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authorjaseg <git@jaseg.de>2021-04-08 14:06:57 +0200
committerjaseg <git@jaseg.de>2021-04-08 14:06:57 +0200
commit870521e698f42a626844e2f5cbeab37a3eeeab4a (patch)
tree9221551fa29c79316a7045c8b14f3a83a82f93fb /doc
parent2a73cef250dd9370c605c0ba185f47eb4b6074d0 (diff)
downloadihsm-870521e698f42a626844e2f5cbeab37a3eeeab4a.tar.gz
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ihsm-870521e698f42a626844e2f5cbeab37a3eeeab4a.zip
Repo re-org: move doc/paper to top level
Diffstat (limited to 'doc')
-rw-r--r--doc/paper/.gitignore10
-rwxr-xr-xdoc/paper/CC-by.eps2727
-rwxr-xr-xdoc/paper/CC-by.pdfbin4153 -> 0 bytes
-rw-r--r--doc/paper/Makefile35
-rw-r--r--doc/paper/circuits.ipynb1115
-rw-r--r--doc/paper/concept_vis_one_axis.pdfbin6623 -> 0 bytes
-rw-r--r--doc/paper/concept_vis_one_axis.svg344
-rwxr-xr-xdoc/paper/goette_inertial_hsms_v1_5_eprint.pdfbin112344 -> 0 bytes
-rwxr-xr-xdoc/paper/iacrtrans.cls448
-rwxr-xr-xdoc/paper/ihsm_shaft_countermeasures_a.pdfbin1486 -> 0 bytes
-rwxr-xr-xdoc/paper/ihsm_shaft_countermeasures_a.svg160
-rwxr-xr-xdoc/paper/ihsm_shaft_countermeasures_b.pdfbin1597 -> 0 bytes
-rwxr-xr-xdoc/paper/ihsm_shaft_countermeasures_b.svg174
-rwxr-xr-xdoc/paper/ihsm_shaft_countermeasures_c.pdfbin1806 -> 0 bytes
-rwxr-xr-xdoc/paper/ihsm_shaft_countermeasures_c.svg246
-rw-r--r--doc/paper/ir_tx_schema.pdfbin4112 -> 0 bytes
-rw-r--r--doc/paper/ir_tx_schema.svg340
-rw-r--r--doc/paper/mesh_gen_viz.pdfbin6880 -> 0 bytes
-rw-r--r--doc/paper/mesh_gen_viz.svg1547
-rw-r--r--doc/paper/mesh_scan_crop.jpgbin400578 -> 0 bytes
-rw-r--r--doc/paper/photolink_schematic.pdfbin15968 -> 0 bytes
-rw-r--r--doc/paper/photolink_schematic.pro43
-rw-r--r--doc/paper/photolink_schematic.sch486
-rw-r--r--doc/paper/photolink_schematic.svg3246
-rw-r--r--doc/paper/proto_3d_design.jpgbin63447 -> 0 bytes
-rw-r--r--doc/paper/prototype_early_comms_small.jpgbin518517 -> 0 bytes
-rw-r--r--doc/paper/prototype_pic.jpgbin1391843 -> 0 bytes
-rw-r--r--doc/paper/prototype_pic2.jpgbin1466004 -> 0 bytes
-rw-r--r--doc/paper/rotohsm.bib249
-rw-r--r--doc/paper/rotohsm_paper.pdfbin3564423 -> 0 bytes
-rw-r--r--doc/paper/rotohsm_paper.tex742
-rw-r--r--doc/paper/rotohsm_tech_report.pdfbin112288 -> 0 bytes
-rw-r--r--doc/paper/rotohsm_tech_report.tex300
-rw-r--r--doc/paper/rotor_stator.jpgbin1031734 -> 0 bytes
34 files changed, 0 insertions, 12212 deletions
diff --git a/doc/paper/.gitignore b/doc/paper/.gitignore
deleted file mode 100644
index c49262e..0000000
--- a/doc/paper/.gitignore
+++ /dev/null
@@ -1,10 +0,0 @@
-*.out
-*.bbl
-*.aux
-*.toc
-*.blg
-*.bcf
-*.log
-*.run.xml
-
-version.tex
diff --git a/doc/paper/CC-by.eps b/doc/paper/CC-by.eps
deleted file mode 100755
index ae05c8b..0000000
--- a/doc/paper/CC-by.eps
+++ /dev/null
@@ -1,2727 +0,0 @@
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- sourcearray 0 get exec
- XIBuffer3
- dup 3 1 roll
-
- /ci6putrgbtograystr load exch
- ci6walkrgbstring
- end
-} def
-/ci6cmyktograyproc {
- Adobe_ColorImage_AI6_Vars begin
- sourcearray 0 get exec
- XIBuffer3
- dup 3 1 roll
-
- /ci6putcmyktograystr load exch
- ci6walkcmykstring
- end
-} def
-/ci6separatecmykproc {
- Adobe_ColorImage_AI6_Vars begin
- sourcearray 0 get exec
-
- XIBuffer3
-
- 0 2 index
-
- plateindex 4 2 index length 1 sub {
- get 255 exch sub
-
- 3 copy put pop 1 add
-
- 2 index
- } for
- pop pop exch pop
- end
-} def
-
-/ci6compositeimage {
- dup 1 eq {
- pop pop image
- }{
- /ci6colorimage load null ne {
- ci6colorimage
- }{
- 3 1 roll pop
- sourcearray 0 3 -1 roll put
- 3 eq {/ci6rgbtograyproc}{/ci6cmyktograyproc} ifelse load
- image
- } ifelse
- } ifelse
-} def
-/ci6knockoutimage {
- gsave
- 0 ci6curtransfer exec 1 ci6curtransfer exec
- eq {
- 0 ci6curtransfer exec 0.5 lt
- }{
- 0 ci6curtransfer exec 1 ci6curtransfer exec gt
- } ifelse
- {{pop 0}}{{pop 1}} ifelse
- systemdict /settransfer get exec
- ci6compositeimage
- grestore
-} def
-/ci6drawimage {
- ci6testplate -1 eq {
- pop ci6compositeimage
- }{
- dup type /arraytype eq {
- dup length plateindex gt {plateindex get}{pop false} ifelse
- }{
- {
- true
- }{
- dup 1 eq {plateindex 3 eq}{plateindex 3 le} ifelse
- } ifelse
- } ifelse
- {
- dup 1 eq {
- pop pop ci6image
- }{
- dup 3 eq {
- ci6compositeimage
- }{
- pop pop
- sourcearray 0 3 -1 roll put
- /ci6separatecmykproc load
- ci6image
- } ifelse
- } ifelse
- }{
- ci6curoverprint {
- 7 {pop} repeat
- }{
- ci6knockoutimage
- } ifelse
- } ifelse
- } ifelse
-} def
-/ci6proctintimage {
- /_ptispace exch store /_ptiname exch store /_pti1 exch store /_pti0 exch store /_ptiproc exch store
- /_pticomps _ptispace ci6numcomps store
- /_ptiscale _pti1 _pti0 sub store
- level2? {
- _ptiname length 0 gt version cvr 2012 ge and {
- [/Separation _ptiname _ptispace {_ptiproc}] setcolorspace
- [_pti0 _pti1] ci6makeimagedict ci6image
- }{
- [/Indexed _ptispace 255 {255 div _ptiscale mul _pti0 add _ptiproc}] setcolorspace
- [0 255] ci6makeimagedict ci6image
- } ifelse
- }{
- _pticomps 1 eq {
- {
- dup
- {
- 255 div _ptiscale mul _pti0 add _ptiproc 255 mul cvi put
- } ci6stringapply
- } ci6concatprocs ci6image
- }{
- {
- dup length _pticomps mul dup _ptibuf length ne {/_ptibuf exch string store}{pop} ifelse
- _ptibuf {
- exch _pticomps mul exch 255 div _ptiscale mul _pti0 add _ptiproc
- _pticomps 2 add -2 roll
- _pticomps 1 sub -1 0 {
- 1 index add 2 index exch
- 5 -1 roll
- 255 mul cvi put
- } for
- pop pop
- } ci6stringapply
- } ci6concatprocs false _pticomps
- /ci6colorimage load null eq {7 {pop} repeat}{ci6colorimage} ifelse
- } ifelse
- } ifelse
-} def
-/ci6graytintimage {
- /_gtigray 5 -1 roll store
- {1 _gtigray sub mul 1 exch sub} 4 1 roll
- /DeviceGray ci6proctintimage
-} def
-/ci6cmyktintimage {
- /_cticmyk 5 -1 roll store
- {_cticmyk {1 index mul exch} forall pop} 4 1 roll
- /DeviceCMYK ci6proctintimage
-} def
-/ci6rgbtintimage {
- /_rtirgb 5 -1 roll store
- {_rtirgb {1 exch sub 1 index mul 1 exch sub exch} forall pop} 4 1 roll
- /DeviceRGB ci6proctintimage
-} def
-/ci6tintimage {
- ci6testplate -1 eq {
- ci6colorexpand
- 3 -1 roll 5 -1 roll {0}{0 exch} ifelse 4 2 roll
- dup /DeviceGray eq {
- pop ci6graytintimage
- }{
- dup /DeviceRGB eq {
- pop ci6rgbtintimage
- }{
- pop ci6cmyktintimage
- } ifelse
- } ifelse
- }{
- dup ci6marksplate {
- plateindex 5 lt {
- ci6colortocmyk plateindex get
- dup 0 eq ci6curoverprint and {
- 7 {pop} repeat
- }{
- 1 exch sub
- exch {1 0}{0 1} ifelse () ci6graytintimage
- } ifelse
- }{
- pop exch {0}{0 exch} ifelse 0 3 1 roll () ci6graytintimage
- } ifelse
- }{
- ci6curoverprint {
- 8 {pop} repeat
- }{
- pop pop pop
- {pop 1} 0 1 () /DeviceGray ci6proctintimage
- } ifelse
- } ifelse
- } ifelse
-} def
-/XINullImage {
-} def
-/XIImageMask {
- XIImageWidth XIImageHeight false
- [XIImageWidth 0 0 XIImageHeight neg 0 0]
- /XIDataProc load
- imagemask
-} def
-/XIImageTint {
- XIImageWidth XIImageHeight XIBitsPerPixel
- [XIImageWidth 0 0 XIImageHeight neg 0 0]
- /XIDataProc load
- XIType 3 eq XIColorValues XIColorSpace ci6tintimage
-} def
-/XIImage {
- XIImageWidth XIImageHeight XIBitsPerPixel
- [XIImageWidth 0 0 XIImageHeight neg 0 0]
- /XIDataProc load
- false XIChannelCount XIPlateList ci6drawimage
-} def
-/XG {
- pop pop
-} def
-/XF {
- 13 {pop} repeat
-} def
-/Xh {
- Adobe_ColorImage_AI6_Vars begin
- gsave
- /XIType exch def
- /XIImageHeight exch def
- /XIImageWidth exch def
- /XIImageMatrix exch def
- 0 0 moveto
- XIImageMatrix concat
- XIImageWidth XIImageHeight scale
-
- /_lp /null ddef
- _fc
- /_lp /imagemask ddef
- end
-} def
-/XH {
- Adobe_ColorImage_AI6_Vars begin
- grestore
- end
-} def
-/XIEnable {
- Adobe_ColorImage_AI6_Vars /XIEnable 3 -1 roll put
-} def
-/XC {
- Adobe_ColorImage_AI6_Vars begin
- ci6colormake
- /XIColorSpace exch def
- /XIColorValues exch def
- end
-} def
-/XIPlates {
- Adobe_ColorImage_AI6_Vars begin
- /XIPlateList exch def
- end
-} def
-/XI
-{
- Adobe_ColorImage_AI6_Vars begin
- gsave
- /XIType exch def
- cvi dup
- 256 idiv /XICompression exch store
- 256 mod /XIEncoding exch store
- pop pop
- /XIChannelCount exch def
- /XIBitsPerPixel exch def
- /XIImageHeight exch def
- /XIImageWidth exch def
- pop pop pop pop
- /XIImageMatrix exch def
- XIBitsPerPixel 1 eq {
- XIImageWidth 8 div ceiling cvi
- }{
- XIImageWidth XIChannelCount mul
- } ifelse
- /XIRowBytes exch def
- XIEnable {
- /XIBuffer3 XIImageWidth string def
- XICompression 0 eq {
- /XIBuffer1 XIRowBytes string def
- XIEncoding 0 eq {
- {currentfile XIBuffer1 readhexstring pop}
- }{
- {currentfile XIBuffer1 readstring pop}
- } ifelse
- }{
- /XIBuffer1 256 string def
- /XIBuffer2 XIRowBytes string def
- {currentfile XIBuffer1 readline pop (%) anchorsearch {pop} if}
- /ASCII85Decode filter /DCTDecode filter
- /XIFile exch def
- {XIFile XIBuffer2 readstring pop}
- } ifelse
- /XIDataProc exch def
-
- XIType 1 ne {
- 0 setgray
- } if
- XIType 1 eq {
- XIImageMask
- }{
- XIType 2 eq XIType 3 eq or {
- XIImageTint
- }{
- XIImage
- } ifelse
- } ifelse
- }{
- XINullImage
- } ifelse
- /XIPlateList false def
- grestore
- end
-} def
-end
-%%EndProcSet
-%%BeginResource: procset Adobe_Illustrator_AI5 1.3 0
-%%Title: (Adobe Illustrator (R) Version 8.0 Full Prolog)
-%%Version: 1.3 0
-%%CreationDate: (3/7/1994) ()
-%%Copyright: ((C) 1987-1998 Adobe Systems Incorporated All Rights Reserved)
-currentpacking true setpacking
-userdict /Adobe_Illustrator_AI5_vars 112 dict dup begin
-put
-/_?cmyk false def
-/_eo false def
-/_lp /none def
-/_pf
-{
-} def
-/_ps
-{
-} def
-/_psf
-{
-} def
-/_pss
-{
-} def
-/_pjsf
-{
-} def
-/_pjss
-{
-} def
-/_pola 0 def
-/_doClip 0 def
-/cf currentflat def
-/_lineorientation 0 def
-/_charorientation 0 def
-/_yokoorientation 0 def
-/_tm matrix def
-/_renderStart
-[
-/e0 /r0 /a0 /o0 /e1 /r1 /a1 /i0
-] def
-/_renderEnd
-[
-null null null null /i1 /i1 /i1 /i1
-] def
-/_render -1 def
-/_shift [0 0] def
-/_ax 0 def
-/_ay 0 def
-/_cx 0 def
-/_cy 0 def
-/_leading
-[
-0 0
-] def
-/_ctm matrix def
-/_mtx matrix def
-/_sp 16#020 def
-/_hyphen (-) def
-/_fontSize 0 def
-/_fontAscent 0 def
-/_fontDescent 0 def
-/_fontHeight 0 def
-/_fontRotateAdjust 0 def
-/Ss 256 string def
-Ss 0 (fonts/) putinterval
-/_cnt 0 def
-/_scale [1 1] def
-/_nativeEncoding 0 def
-/_useNativeEncoding 0 def
-/_tempEncode 0 def
-/_pntr 0 def
-/_tDict 2 dict def
-/_hfname 100 string def
-/_hffound false def
-/Tx
-{
-} def
-/Tj
-{
-} def
-/CRender
-{
-} def
-/_AI3_savepage
-{
-} def
-/_gf null def
-/_cf 4 array def
-/_rgbf 3 array def
-/_if null def
-/_of false def
-/_fc
-{
-} def
-/_gs null def
-/_cs 4 array def
-/_rgbs 3 array def
-/_is null def
-/_os false def
-/_sc
-{
-} def
-/_pd 1 dict def
-/_ed 15 dict def
-/_pm matrix def
-/_fm null def
-/_fd null def
-/_fdd null def
-/_sm null def
-/_sd null def
-/_sdd null def
-/_i null def
-/_lobyte 0 def
-/_hibyte 0 def
-/_cproc null def
-/_cscript 0 def
-/_hvax 0 def
-/_hvay 0 def
-/_hvwb 0 def
-/_hvcx 0 def
-/_hvcy 0 def
-/_bitfont null def
-/_bitlobyte 0 def
-/_bithibyte 0 def
-/_bitkey null def
-/_bitdata null def
-/_bitindex 0 def
-/discardSave null def
-/buffer 256 string def
-/beginString null def
-/endString null def
-/endStringLength null def
-/layerCnt 1 def
-/layerCount 1 def
-/perCent (%) 0 get def
-/perCentSeen? false def
-/newBuff null def
-/newBuffButFirst null def
-/newBuffLast null def
-/clipForward? false def
-end
-userdict /Adobe_Illustrator_AI5 known not {
- userdict /Adobe_Illustrator_AI5 100 dict put
-} if
-userdict /Adobe_Illustrator_AI5 get begin
-/initialize
-{
- Adobe_Illustrator_AI5 dup begin
- Adobe_Illustrator_AI5_vars begin
- /_aicmykps where {pop /_?cmyk _aicmykps def}if
- discardDict
- {
- bind pop pop
- } forall
- dup /nc get begin
- {
- dup xcheck 1 index type /operatortype ne and
- {
- bind
- } if
- pop pop
- } forall
- end
- newpath
-} def
-/terminate
-{
- end
- end
-} def
-/_
-null def
-/ddef
-{
- Adobe_Illustrator_AI5_vars 3 1 roll put
-} def
-/xput
-{
- dup load dup length exch maxlength eq
- {
- dup dup load dup
- length 2 mul dict copy def
- } if
- load begin
- def
- end
-} def
-/npop
-{
- {
- pop
- } repeat
-} def
-/hswj
-{
- dup stringwidth 3 2 roll
- {
- _hvwb eq { exch _hvcx add exch _hvcy add } if
- exch _hvax add exch _hvay add
- } cforall
-} def
-/vswj
-{
- 0 0 3 -1 roll
- {
- dup 255 le
- _charorientation 1 eq
- and
- {
- dup cstring stringwidth 5 2 roll
- _hvwb eq { exch _hvcy sub exch _hvcx sub } if
- exch _hvay sub exch _hvax sub
- 4 -1 roll sub exch
- 3 -1 roll sub exch
- }
- {
- _hvwb eq { exch _hvcy sub exch _hvcx sub } if
- exch _hvay sub exch _hvax sub
- _fontHeight sub
- } ifelse
- } cforall
-} def
-/swj
-{
- 6 1 roll
- /_hvay exch ddef
- /_hvax exch ddef
- /_hvwb exch ddef
- /_hvcy exch ddef
- /_hvcx exch ddef
- _lineorientation 0 eq { hswj } { vswj } ifelse
-} def
-/sw
-{
- 0 0 0 6 3 roll swj
-} def
-/vjss
-{
- 4 1 roll
- {
- dup cstring
- dup length 1 eq
- _charorientation 1 eq
- and
- {
- -90 rotate
- currentpoint
- _fontRotateAdjust add
- moveto
- gsave
- false charpath currentpoint
- 5 index setmatrix stroke
- grestore
- _fontRotateAdjust sub
- moveto
- _sp eq
- {
- 5 index 5 index rmoveto
- } if
- 2 copy rmoveto
- 90 rotate
- }
- {
- currentpoint
- _fontHeight sub
- 5 index sub
- 3 index _sp eq
- {
- 9 index sub
- } if
-
- currentpoint
- exch 4 index stringwidth pop 2 div sub
- exch _fontAscent sub
- moveto
-
- gsave
- 2 index false charpath
- 6 index setmatrix stroke
- grestore
-
- moveto pop pop
- } ifelse
- } cforall
- 6 npop
-} def
-/hjss
-{
- 4 1 roll
- {
- dup cstring
- gsave
- false charpath currentpoint
- 5 index setmatrix stroke
- grestore
- moveto
- _sp eq
- {
- 5 index 5 index rmoveto
- } if
- 2 copy rmoveto
- } cforall
- 6 npop
-} def
-/jss
-{
- _lineorientation 0 eq { hjss } { vjss } ifelse
-} def
-/ss
-{
- 0 0 0 7 3 roll jss
-} def
-/vjsp
-{
- 4 1 roll
- {
- dup cstring
- dup length 1 eq
- _charorientation 1 eq
- and
- {
- -90 rotate
- currentpoint
- _fontRotateAdjust add
- moveto
- false charpath
- currentpoint
- _fontRotateAdjust sub
- moveto
- _sp eq
- {
- 5 index 5 index rmoveto
- } if
- 2 copy rmoveto
- 90 rotate
- }
- {
- currentpoint
- _fontHeight sub
- 5 index sub
- 3 index _sp eq
- {
- 9 index sub
- } if
-
- currentpoint
- exch 4 index stringwidth pop 2 div sub
- exch _fontAscent sub
- moveto
-
- 2 index false charpath
-
- moveto pop pop
- } ifelse
- } cforall
- 6 npop
-} def
-/hjsp
-{
- 4 1 roll
- {
- dup cstring
- false charpath
- _sp eq
- {
- 5 index 5 index rmoveto
- } if
- 2 copy rmoveto
- } cforall
- 6 npop
-} def
-/jsp
-{
- matrix currentmatrix
- _lineorientation 0 eq {hjsp} {vjsp} ifelse
-} def
-/sp
-{
- matrix currentmatrix
- 0 0 0 7 3 roll
- _lineorientation 0 eq {hjsp} {vjsp} ifelse
-} def
-/pl
-{
- transform
- 0.25 sub round 0.25 add exch
- 0.25 sub round 0.25 add exch
- itransform
-} def
-/setstrokeadjust where
-{
- pop true setstrokeadjust
- /c
- {
- curveto
- } def
- /C
- /c load def
- /v
- {
- currentpoint 6 2 roll curveto
- } def
- /V
- /v load def
- /y
- {
- 2 copy curveto
- } def
- /Y
- /y load def
- /l
- {
- lineto
- } def
- /L
- /l load def
- /m
- {
- moveto
- } def
-}
-{
- /c
- {
- pl curveto
- } def
- /C
- /c load def
- /v
- {
- currentpoint 6 2 roll pl curveto
- } def
- /V
- /v load def
- /y
- {
- pl 2 copy curveto
- } def
- /Y
- /y load def
- /l
- {
- pl lineto
- } def
- /L
- /l load def
- /m
- {
- pl moveto
- } def
-} ifelse
-/d
-{
- setdash
-} def
-/cf
-{
-} def
-/i
-{
- dup 0 eq
- {
- pop cf
- } if
- setflat
-} def
-/j
-{
- setlinejoin
-} def
-/J
-{
- setlinecap
-} def
-/M
-{
- setmiterlimit
-} def
-/w
-{
- setlinewidth
-} def
-/XR
-{
- 0 ne
- /_eo exch ddef
-} def
-/H
-{
-} def
-/h
-{
- closepath
-} def
-/N
-{
- _pola 0 eq
- {
- _doClip 1 eq
- {
- _eo {eoclip} {clip} ifelse /_doClip 0 ddef
- } if
- newpath
- }
- {
- /CRender
- {
- N
- } ddef
- } ifelse
-} def
-/n
-{
- N
-} def
-/F
-{
- _pola 0 eq
- {
- _doClip 1 eq
- {
- gsave _pf grestore _eo {eoclip} {clip} ifelse newpath /_lp /none ddef _fc
- /_doClip 0 ddef
- }
- {
- _pf
- } ifelse
- }
- {
- /CRender
- {
- F
- } ddef
- } ifelse
-} def
-/f
-{
- closepath
- F
-} def
-/S
-{
- _pola 0 eq
- {
- _doClip 1 eq
- {
- gsave _ps grestore _eo {eoclip} {clip} ifelse newpath /_lp /none ddef _sc
- /_doClip 0 ddef
- }
- {
- _ps
- } ifelse
- }
- {
- /CRender
- {
- S
- } ddef
- } ifelse
-} def
-/s
-{
- closepath
- S
-} def
-/B
-{
- _pola 0 eq
- {
- _doClip 1 eq
- gsave F grestore
- {
- gsave S grestore _eo {eoclip} {clip} ifelse newpath /_lp /none ddef _sc
- /_doClip 0 ddef
- }
- {
- S
- } ifelse
- }
- {
- /CRender
- {
- B
- } ddef
- } ifelse
-} def
-/b
-{
- closepath
- B
-} def
-/W
-{
- /_doClip 1 ddef
-} def
-/*
-{
- count 0 ne
- {
- dup type /stringtype eq
- {
- pop
- } if
- } if
- newpath
-} def
-/u
-{
-} def
-/U
-{
-} def
-/q
-{
- _pola 0 eq
- {
- gsave
- } if
-} def
-/Q
-{
- _pola 0 eq
- {
- grestore
- } if
-} def
-/*u
-{
- _pola 1 add /_pola exch ddef
-} def
-/*U
-{
- _pola 1 sub /_pola exch ddef
- _pola 0 eq
- {
- CRender
- } if
-} def
-/D
-{
- pop
-} def
-/*w
-{
-} def
-/*W
-{
-} def
-/`
-{
- /_i save ddef
- clipForward?
- {
- nulldevice
- } if
- 6 1 roll 4 npop
- concat pop
- userdict begin
- /showpage
- {
- } def
- 0 setgray
- 0 setlinecap
- 1 setlinewidth
- 0 setlinejoin
- 10 setmiterlimit
- [] 0 setdash
- /setstrokeadjust where {pop false setstrokeadjust} if
- newpath
- 0 setgray
- false setoverprint
-} def
-/~
-{
- end
- _i restore
-} def
-/_rgbtocmyk
-{
- 3
- {
- 1 exch sub 3 1 roll
- } repeat
- 3 copy 1 4 1 roll
- 3
- {
- 3 index 2 copy gt
- {
- exch
- } if
- pop 4 1 roll
- } repeat
- pop pop pop
- 4 1 roll
- 3
- {
- 3 index sub
- 3 1 roll
- } repeat
- 4 -1 roll
-} def
-/setrgbfill
-{
- _rgbf astore pop
- /_fc
- {
- _lp /fill ne
- {
- _of setoverprint
- _rgbf aload pop setrgbcolor
- /_lp /fill ddef
- } if
- } ddef
- /_pf
- {
- _fc
- _eo {eofill} {fill} ifelse
- } ddef
- /_psf
- {
- _fc
- hvashow
- } ddef
- /_pjsf
- {
- _fc
- hvawidthshow
- } ddef
- /_lp /none ddef
-} def
-/setrgbstroke
-{
- _rgbs astore pop
- /_sc
- {
- _lp /stroke ne
- {
- _os setoverprint
- _rgbs aload pop setrgbcolor
- /_lp /stroke ddef
- } if
- } ddef
- /_ps
- {
- _sc
- stroke
- } ddef
- /_pss
- {
- _sc
- ss
- } ddef
- /_pjss
- {
- _sc
- jss
- } ddef
- /_lp /none ddef
-} def
-/O
-{
- 0 ne
- /_of exch ddef
- /_lp /none ddef
-} def
-/R
-{
- 0 ne
- /_os exch ddef
- /_lp /none ddef
-} def
-/g
-{
- /_gf exch ddef
- /_fc
- {
- _lp /fill ne
- {
- _of setoverprint
- _gf setgray
- /_lp /fill ddef
- } if
- } ddef
- /_pf
- {
- _fc
- _eo {eofill} {fill} ifelse
- } ddef
- /_psf
- {
- _fc
- hvashow
- } ddef
- /_pjsf
- {
- _fc
- hvawidthshow
- } ddef
- /_lp /none ddef
-} def
-/G
-{
- /_gs exch ddef
- /_sc
- {
- _lp /stroke ne
- {
- _os setoverprint
- _gs setgray
- /_lp /stroke ddef
- } if
- } ddef
- /_ps
- {
- _sc
- stroke
- } ddef
- /_pss
- {
- _sc
- ss
- } ddef
- /_pjss
- {
- _sc
- jss
- } ddef
- /_lp /none ddef
-} def
-/k
-{
- _cf astore pop
- /_fc
- {
- _lp /fill ne
- {
- _of setoverprint
- _cf aload pop setcmykcolor
- /_lp /fill ddef
- } if
- } ddef
- /_pf
- {
- _fc
- _eo {eofill} {fill} ifelse
- } ddef
- /_psf
- {
- _fc
- hvashow
- } ddef
- /_pjsf
- {
- _fc
- hvawidthshow
- } ddef
- /_lp /none ddef
-} def
-/K
-{
- _cs astore pop
- /_sc
- {
- _lp /stroke ne
- {
- _os setoverprint
- _cs aload pop setcmykcolor
- /_lp /stroke ddef
- } if
- } ddef
- /_ps
- {
- _sc
- stroke
- } ddef
- /_pss
- {
- _sc
- ss
- } ddef
- /_pjss
- {
- _sc
- jss
- } ddef
- /_lp /none ddef
-} def
-/Xa
-{
- _?cmyk {
- 3 npop k
- }{
- setrgbfill 4 npop
- } ifelse
-} def
-/XA
-{
- _?cmyk {
- 3 npop K
- }{
- setrgbstroke 4 npop
- } ifelse
-} def
-/Xs
-{
- /_gf exch ddef
- 5 npop
- /_fc
- {
- _lp /fill ne
- {
- _of setoverprint
- _gf setAIseparationgray
- /_lp /fill ddef
- } if
- } ddef
- /_pf
- {
- _fc
- _eo {eofill} {fill} ifelse
- } ddef
- /_psf
- {
- _fc
- hvashow
- } ddef
- /_pjsf
- {
- _fc
- hvawidthshow
- } ddef
- /_lp /none ddef
-} def
-/XS
-{
- /_gs exch ddef
- 5 npop
- /_sc
- {
- _lp /stroke ne
- {
- _os setoverprint
- _gs setAIseparationgray
- /_lp /stroke ddef
- } if
- } ddef
- /_ps
- {
- _sc
- stroke
- } ddef
- /_pss
- {
- _sc
- ss
- } ddef
- /_pjss
- {
- _sc
- jss
- } ddef
- /_lp /none ddef
-} def
-/Xx
-{
- exch
- /_gf exch ddef
- 0 eq {
- findcmykcustomcolor
- }{
- _?cmyk {true}{/findrgbcustomcolor where{pop false}{true}ifelse}ifelse
- {
- 4 1 roll 3 npop
- findcmykcustomcolor
- }{
- 8 -4 roll 4 npop
- findrgbcustomcolor
- } ifelse
- } ifelse
- /_if exch ddef
- /_fc
- {
- _lp /fill ne
- {
- _of setoverprint
- _if _gf 1 exch sub setcustomcolor
- /_lp /fill ddef
- } if
- } ddef
- /_pf
- {
- _fc
- _eo {eofill} {fill} ifelse
- } ddef
- /_psf
- {
- _fc
- hvashow
- } ddef
- /_pjsf
- {
- _fc
- hvawidthshow
- } ddef
- /_lp /none ddef
-} def
-/XX
-{
- exch
- /_gs exch ddef
- 0 eq {
- findcmykcustomcolor
- }{
- _?cmyk {true}{/findrgbcustomcolor where{pop false}{true}ifelse}ifelse
- {
- 4 1 roll 3 npop
- findcmykcustomcolor
- }{
- 8 -4 roll 4 npop
- findrgbcustomcolor
- } ifelse
- } ifelse
- /_is exch ddef
- /_sc
- {
- _lp /stroke ne
- {
- _os setoverprint
- _is _gs 1 exch sub setcustomcolor
- /_lp /stroke ddef
- } if
- } ddef
- /_ps
- {
- _sc
- stroke
- } ddef
- /_pss
- {
- _sc
- ss
- } ddef
- /_pjss
- {
- _sc
- jss
- } ddef
- /_lp /none ddef
-} def
-/x
-{
- /_gf exch ddef
- findcmykcustomcolor
- /_if exch ddef
- /_fc
- {
- _lp /fill ne
- {
- _of setoverprint
- _if _gf 1 exch sub setcustomcolor
- /_lp /fill ddef
- } if
- } ddef
- /_pf
- {
- _fc
- _eo {eofill} {fill} ifelse
- } ddef
- /_psf
- {
- _fc
- hvashow
- } ddef
- /_pjsf
- {
- _fc
- hvawidthshow
- } ddef
- /_lp /none ddef
-} def
-/X
-{
- /_gs exch ddef
- findcmykcustomcolor
- /_is exch ddef
- /_sc
- {
- _lp /stroke ne
- {
- _os setoverprint
- _is _gs 1 exch sub setcustomcolor
- /_lp /stroke ddef
- } if
- } ddef
- /_ps
- {
- _sc
- stroke
- } ddef
- /_pss
- {
- _sc
- ss
- } ddef
- /_pjss
- {
- _sc
- jss
- } ddef
- /_lp /none ddef
-} def
-/XK
-{
- 3 -1 roll pop
- 0 eq
- {
- 1 exch sub
- 3 {dup 3 1 roll mul 5 1 roll} repeat
- mul 4 1 roll
- K
- }
- {
- 1 exch sub 4 1 roll
- 3 {1 exch sub 3 index mul 1 exch sub 3 1 roll} repeat
- 4 -1 roll pop
- XA
- } ifelse
-} def
-/Xk
-{
- 3 -1 roll pop
- 0 eq
- {
- 1 exch sub
- 3 {dup 3 1 roll mul 5 1 roll} repeat
- mul 4 1 roll
- k
- }
- {
- 1 exch sub 4 1 roll
- 3 {1 exch sub 3 index mul 1 exch sub 3 1 roll} repeat
- 4 -1 roll pop
- Xa
- } ifelse
-} def
-/A
-{
- pop
-} def
-/annotatepage
-{
-userdict /annotatepage 2 copy known {get exec} {pop pop} ifelse
-} def
-/XT {
- pop pop
-} def
-/Xt {
- pop
-} def
-/discard
-{
- save /discardSave exch store
- discardDict begin
- /endString exch store
- gt38?
- {
- 2 add
- } if
- load
- stopped
- pop
- end
- discardSave restore
-} bind def
-userdict /discardDict 7 dict dup begin
-put
-/pre38Initialize
-{
- /endStringLength endString length store
- /newBuff buffer 0 endStringLength getinterval store
- /newBuffButFirst newBuff 1 endStringLength 1 sub getinterval store
- /newBuffLast newBuff endStringLength 1 sub 1 getinterval store
-} def
-/shiftBuffer
-{
- newBuff 0 newBuffButFirst putinterval
- newBuffLast 0
- currentfile read not
- {
- stop
- } if
- put
-} def
-0
-{
- pre38Initialize
- mark
- currentfile newBuff readstring exch pop
- {
- {
- newBuff endString eq
- {
- cleartomark stop
- } if
- shiftBuffer
- } loop
- }
- {
- stop
- } ifelse
-} def
-1
-{
- pre38Initialize
- /beginString exch store
- mark
- currentfile newBuff readstring exch pop
- {
- {
- newBuff beginString eq
- {
- /layerCount dup load 1 add store
- }
- {
- newBuff endString eq
- {
- /layerCount dup load 1 sub store
- layerCount 0 eq
- {
- cleartomark stop
- } if
- } if
- } ifelse
- shiftBuffer
- } loop
- } if
-} def
-2
-{
- mark
- {
- currentfile buffer {readline} stopped {
- % assume error was due to overfilling the buffer
- }{
- not
- {
- stop
- } if
- endString eq {
- cleartomark stop
- } if
- }ifelse
- } loop
-} def
-3
-{
- /beginString exch store
- /layerCnt 1 store
- mark
- {
- currentfile buffer {readline} stopped {
- % assume error was due to overfilling the buffer
- }{
- not
- {
- stop
- } if
- dup beginString eq
- {
- pop /layerCnt dup load 1 add store
- }
- {
- endString eq
- {
- layerCnt 1 eq
- {
- cleartomark stop
- }
- {
- /layerCnt dup load 1 sub store
- } ifelse
- } if
- } ifelse
- }ifelse
- } loop
-} def
-end
-userdict /clipRenderOff 15 dict dup begin
-put
-{
- /n /N /s /S /f /F /b /B
-}
-{
- {
- _doClip 1 eq
- {
- /_doClip 0 ddef _eo {eoclip} {clip} ifelse
- } if
- newpath
- } def
-} forall
-/Tr /pop load def
-/Bb {} def
-/BB /pop load def
-/Bg {12 npop} def
-/Bm {6 npop} def
-/Bc /Bm load def
-/Bh {4 npop} def
-end
-/Lb
-{
- 6 npop
- 7 2 roll
- 5 npop
- 0 eq
- {
- 0 eq
- {
- (%AI5_BeginLayer) 1 (%AI5_EndLayer--) discard
- }
- {
-
- /clipForward? true def
-
- /Tx /pop load def
- /Tj /pop load def
-
- currentdict end clipRenderOff begin begin
- } ifelse
- }
- {
- 0 eq
- {
- save /discardSave exch store
- } if
- } ifelse
-} bind def
-/LB
-{
- discardSave dup null ne
- {
- restore
- }
- {
- pop
- clipForward?
- {
- currentdict
- end
- end
- begin
-
- /clipForward? false ddef
- } if
- } ifelse
-} bind def
-/Pb
-{
- pop pop
- 0 (%AI5_EndPalette) discard
-} bind def
-/Np
-{
- 0 (%AI5_End_NonPrinting--) discard
-} bind def
-/Ln /pop load def
-/Ap
-/pop load def
-/Ar
-{
- 72 exch div
- 0 dtransform dup mul exch dup mul add sqrt
- dup 1 lt
- {
- pop 1
- } if
- setflat
-} def
-/Mb
-{
- q
-} def
-/Md
-{
-} def
-/MB
-{
- Q
-} def
-/nc 4 dict def
-nc begin
-/setgray
-{
- pop
-} bind def
-/setcmykcolor
-{
- 4 npop
-} bind def
-/setrgbcolor
-{
- 3 npop
-} bind def
-/setcustomcolor
-{
- 2 npop
-} bind def
-currentdict readonly pop
-end
-/XP
-{
- 4 npop
-} bind def
-/XD
-{
- pop
-} bind def
-end
-setpacking
-%%EndResource
-%%BeginResource: procset Adobe_cshow 2.0 8
-%%Title: (Writing System Operators)
-%%Version: 2.0 8
-%%CreationDate: (1/23/89) ()
-%%Copyright: ((C) 1992-1996 Adobe Systems Incorporated All Rights Reserved)
-currentpacking true setpacking
-userdict /Adobe_cshow 14 dict dup begin put
-/initialize
-{
- Adobe_cshow begin
- Adobe_cshow
- {
- dup xcheck
- {
- bind
- } if
- pop pop
- } forall
- end
- Adobe_cshow begin
-} def
-/terminate
-{
-currentdict Adobe_cshow eq
- {
- end
- } if
-} def
-/cforall
-{
- /_lobyte 0 ddef
- /_hibyte 0 ddef
- /_cproc exch ddef
- /_cscript currentfont /FontScript known { currentfont /FontScript get } { -1 } ifelse ddef
- {
- /_lobyte exch ddef
- _hibyte 0 eq
- _cscript 1 eq
- _lobyte 129 ge _lobyte 159 le and
- _lobyte 224 ge _lobyte 252 le and or and
- _cscript 2 eq
- _lobyte 161 ge _lobyte 254 le and and
- _cscript 3 eq
- _lobyte 161 ge _lobyte 254 le and and
- _cscript 25 eq
- _lobyte 161 ge _lobyte 254 le and and
- _cscript -1 eq
- or or or or and
- {
- /_hibyte _lobyte ddef
- }
- {
- _hibyte 256 mul _lobyte add
- _cproc
- /_hibyte 0 ddef
- } ifelse
- } forall
-} def
-/cstring
-{
- dup 256 lt
- {
- (s) dup 0 4 3 roll put
- }
- {
- dup 256 idiv exch 256 mod
- (hl) dup dup 0 6 5 roll put 1 4 3 roll put
- } ifelse
-} def
-/clength
-{
- 0 exch
- { 256 lt { 1 } { 2 } ifelse add } cforall
-} def
-/hawidthshow
-{
- {
- dup cstring
- show
- _hvax _hvay rmoveto
- _hvwb eq { _hvcx _hvcy rmoveto } if
- } cforall
-} def
-/vawidthshow
-{
- {
- dup 255 le
- _charorientation 1 eq
- and
- {
- -90 rotate
- 0 _fontRotateAdjust rmoveto
- cstring
- _hvcx _hvcy _hvwb _hvax _hvay 6 -1 roll awidthshow
- 0 _fontRotateAdjust neg rmoveto
- 90 rotate
- }
- {
- currentpoint
- _fontHeight sub
- exch _hvay sub exch _hvax sub
- 2 index _hvwb eq { exch _hvcy sub exch _hvcx sub } if
- 3 2 roll
- cstring
- dup stringwidth pop 2 div neg _fontAscent neg rmoveto
- show
- moveto
- } ifelse
- } cforall
-} def
-/hvawidthshow
-{
- 6 1 roll
- /_hvay exch ddef
- /_hvax exch ddef
- /_hvwb exch ddef
- /_hvcy exch ddef
- /_hvcx exch ddef
- _lineorientation 0 eq { hawidthshow } { vawidthshow } ifelse
-} def
-/hvwidthshow
-{
- 0 0 3 -1 roll hvawidthshow
-} def
-/hvashow
-{
- 0 0 0 6 -3 roll hvawidthshow
-} def
-/hvshow
-{
- 0 0 0 0 0 6 -1 roll hvawidthshow
-} def
-currentdict readonly pop end
-setpacking
-%%EndResource
-%%BeginResource: procset Adobe_shading_AI8 1.0 0
-%%Title: (Adobe Illustrator 8 Shading Procset)
-%%Version: 1.0 0
-%%CreationDate: (12/17/97) ()
-%%Copyright: ((C) 1987-1997 Adobe Systems Incorporated All Rights Reserved)
-userdict /defaultpacking currentpacking put true setpacking
-userdict /Adobe_shading_AI8 10 dict dup begin put
-/initialize {
- Adobe_shading_AI8 begin
- Adobe_shading_AI8 bdprocs
- Mesh /initialize get exec
-} def
-/terminate {
- currentdict Adobe_shading_AI8 eq {
- end
- } if
-} def
-/bdprocs {
- {
- dup xcheck 1 index type /arraytype eq and {
- bind
- } if
- pop pop
- } forall
-} def
-/X! {pop} def
-/X# {pop pop} def
-/Mesh 40 dict def
-Mesh begin
-/initialize {
- Mesh bdprocs
- Mesh begin
- /emulate? /AI8MeshEmulation where {
- pop AI8MeshEmulation
- }{
- systemdict /shfill known not
- } ifelse def
- end
-} def
-/bd {
- shadingdict begin
-} def
-/paint {
- emulate? {
- end
- }{
- /_lp /none ddef _fc /_lp /none ddef
-
- /AIColorSpace AIColorSpace tocolorspace store
- /ColorSpace AIColorSpace topsspace store
-
- version_ge_3010.106 not systemdict /setsmoothness known and {
- 0.0001 setsmoothness
- } if
-
- composite? {
- /DataSource getdatasrc def
- Matrix concat
- currentdict end
- shfill
- }{
- AIColorSpace makesmarks AIPlateList markingplate and not isoverprint and {
- end
- }{
- /ColorSpace /DeviceGray store
- /Decode [0 1 0 1 0 1] store
- /DataSource getplatesrc def
- Matrix concat
- currentdict end
- shfill
- } ifelse
- } ifelse
- } ifelse
-} def
-/shadingdict 12 dict def
-shadingdict begin
- /ShadingType 6 def
- /BitsPerCoordinate 16 def
- /BitsPerComponent 8 def
- /BitsPerFlag 8 def
-end
-/datafile null def
-/databuf 256 string def
-/dataptr 0 def
-/srcspace null def
-/srcchannels 0 def
-/dstchannels 0 def
-/dstplate 0 def
-/srctodstcolor null def
-/getplatesrc {
- /srcspace AIColorSpace store
- /srcchannels AIColorSpace getnchannels store
- /dstchannels 1 store
- /dstplate getplateindex store
- /srctodstcolor srcspace makesmarks {
- dstplate 4 eq {
- {1 exch sub}
- }{
- {srcspace tocmyk 3 dstplate sub index 1 exch sub 5 1 roll 4 {pop} repeat}
- } ifelse
- }{
- {srcchannels {pop} repeat 1}
- } ifelse store
- /datafile getdatasrc store
- /rdpatch168 load DataLength () /SubFileDecode filter
-} def
-/getdatasrc {
- /rdcmntline load /ASCII85Decode filter
-} def
-/rdpatch168 {
- /dataptr 0 store
- 49 rdcount
- 4 {
- dup {pop srcchannels getint8} if
- dup {pop srctodstcolor dstchannels putint8 true} if
- } repeat
- {databuf 0 dataptr getinterval}{()} ifelse
-} def
-/rdpatch3216 {
- /dataptr 0 store
- 97 rdcount
- 4 {
- dup {pop srcchannels getint16} if
- dup {pop srctodstcolor dstchannels putint16 true} if
- } repeat
- {databuf 0 dataptr getinterval}{()} ifelse
-} def
-/rdcount {
- dup 0 gt {
- datafile databuf dataptr 4 -1 roll getinterval readstring
- exch length dataptr add /dataptr exch store
- }{
- true
- } ifelse
-} def
-/getint8 {
- mark true 3 -1 roll
- {
- dup {pop datafile read} if
- dup {pop 255 div true} if
- } repeat
- {
- counttomark 1 add -1 roll pop true
- }{
- cleartomark false
- } ifelse
-} def
-/putint8 {
- dup dataptr add /dataptr exch store
- dataptr exch
- {
- 1 sub exch
- 255 mul cvi
- databuf 2 index
- 3 -1 roll put
- } repeat
- pop
-} def
-/getint16 {
- mark true 3 -1 roll
- {
- dup {pop datafile read} if
- dup {pop 256 mul datafile read} if
- dup {pop add 65535 div true} if
- } repeat
- {
- counttomark 1 add -1 roll pop true
- }{
- cleartomark false
- } ifelse
-} def
-/putint16 {
- dup 2 mul dataptr add /dataptr exch store
- dataptr exch
- {
- 2 sub exch
- 65535 mul cvi dup
- 256 idiv databuf 3 index 3 -1 roll put
- 256 mod databuf 2 index 1 add 3 -1 roll put
- } repeat
- pop
-} def
-/srcbuf 256 string def
-/rdcmntline {
- currentfile srcbuf readline pop
- (%) anchorsearch {pop} if
-} def
-/getplateindex {
- 0 [cyan? magenta? yellow? black? customColor?] {{exit} if 1 add} forall
-} def
-/aicsarray 4 array def
-/aicsaltvals 4 array def
-/aicsaltcolr aicsaltvals def
-/tocolorspace {
- dup type /arraytype eq {
- mark exch aload pop
- aicsarray 0 3 -1 roll put
- aicsarray 1 3 -1 roll put
- dup aicsarray 2 3 -1 roll put
- gettintxform aicsarray 3 3 -1 roll put
- counttomark aicsaltvals 0 3 -1 roll getinterval /aicsaltcolr exch store
- aicsaltcolr astore pop pop
- aicsarray
- } if
-} def
-/subtintxform {aicsaltcolr {1 index mul exch} forall pop} def
-/addtintxform {aicsaltcolr {1 sub 1 index mul 1 add exch} forall pop} def
-/gettintxform {
- /DeviceRGB eq {/addtintxform}{/subtintxform} ifelse load
-} def
-/getnchannels {
- dup type /arraytype eq {0 get} if
- colorspacedict exch get begin Channels end
-} def
-/makesmarks {
- composite? {
- pop true
- }{
- dup dup type /arraytype eq {0 get} if
- colorspacedict exch get begin MarksPlate end
- } ifelse
-} def
-/markingplate {
- composite? {
- pop true
- }{
- dup type /arraytype eq {
- dup length getplateindex gt {getplateindex get}{pop false} ifelse
- } if
- } ifelse
-} def
-/tocmyk {
- dup dup type /arraytype eq {0 get} if
- colorspacedict exch get begin ToCMYK end
-} def
-/topsspace {
- dup dup type /arraytype eq {0 get} if
- colorspacedict exch get begin ToPSSpace end
-} def
-/colorspacedict 5 dict dup begin
- /DeviceGray 4 dict dup begin
- /Channels 1 def
- /MarksPlate {pop black?} def
- /ToCMYK {pop 1 exch sub 0 0 0 4 -1 roll} def
- /ToPSSpace {} def
- end def
- /DeviceRGB 4 dict dup begin
- /Channels 3 def
- /MarksPlate {pop isCMYKSep?} def
- /ToCMYK {pop _rgbtocmyk} def
- /ToPSSpace {} def
- end def
- /DeviceCMYK 4 dict dup begin
- /Channels 4 def
- /MarksPlate {pop isCMYKSep?} def
- /ToCMYK {pop} def
- /ToPSSpace {} def
- end def
- /Separation 4 dict dup begin
- /Channels 1 def
- /MarksPlate {
- /findcmykcustomcolor where {
- pop dup 1 exch ToCMYK 5 -1 roll 1 get
- findcmykcustomcolor 1 setcustomcolor
- systemdict /currentgray get exec
- 1 ne
- }{
- pop false
- } ifelse
- } def
- /ToCMYK {
- dup 2 get mark exch 4 2 roll
- 3 get exec
- counttomark -1 roll tocmyk
- 5 -1 roll pop
- } def
- /ToPSSpace {} def
- end def
- /Process 4 dict dup begin
- /Channels 1 def
- /MarksPlate {
- isCMYKSep? {
- 1 exch ToCMYK 4 array astore getplateindex get 0 ne
- }{
- pop false
- } ifelse
- } def
- /ToCMYK {
- dup 2 get mark exch 4 2 roll
- 3 get exec
- counttomark -1 roll tocmyk
- 5 -1 roll pop
- } def
- /ToPSSpace {
- 4 array copy dup 0 /Separation put
- } def
- end def
-end def
-/isoverprint {
- /currentoverprint where {pop currentoverprint}{_of} ifelse
-} def
-/version_ge_3010.106 {
- version {cvr} stopped {
- pop
- false
- }{
- 3010.106 ge
- } ifelse
-} def
-end
-end
-defaultpacking setpacking
-%%EndResource
-%%EndProlog %%BeginSetup userdict /_useSmoothShade false put userdict /_aicmykps true put userdict /_forceToCMYK true put Adobe_level2_AI5 /initialize get exec
-Adobe_cshow /initialize get exec
-Adobe_ColorImage_AI6 /initialize get exec
-Adobe_shading_AI8 /initialize get exec
-Adobe_Illustrator_AI5 /initialize get exec
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Adobe_Illustrator_AI5 /terminate get exec
-Adobe_shading_AI8 /terminate get exec
-Adobe_ColorImage_AI6 /terminate get exec
-Adobe_cshow /terminate get exec
-Adobe_level2_AI5 /terminate get exec
-%%EOF \ No newline at end of file
diff --git a/doc/paper/CC-by.pdf b/doc/paper/CC-by.pdf
deleted file mode 100755
index 7b790d0..0000000
--- a/doc/paper/CC-by.pdf
+++ /dev/null
Binary files differ
diff --git a/doc/paper/Makefile b/doc/paper/Makefile
deleted file mode 100644
index 8a4bc75..0000000
--- a/doc/paper/Makefile
+++ /dev/null
@@ -1,35 +0,0 @@
-
-LAB_PATH ?= ../lab-windows
-
-SHELL := bash
-.ONESHELL:
-.SHELLFLAGS := -eu -o pipefail -c
-.DELETE_ON_ERROR:
-MAKEFLAGS += --warn-undefined-variables
-MAKEFLAGS += --no-builtin-rules
-
-main_tex ?= rotohsm_paper
-brief_tex ?= rotohsm_tech_report
-
-VERSION_STRING := $(shell git describe --tags --long --dirty)
-
-all: ${main_tex}.pdf ${brief_tex}.pdf
-
-%.pdf: %.tex rotohsm.bib version.tex
- pdflatex -shell-escape $<
- biber $*
- pdflatex -shell-escape $<
-
-version.tex: ${main_tex}.tex ${brief_tex}.tex rotohsm.bib
- echo "${VERSION_STRING}" > $@
-
-resources/%.pdf: $(LAB_PATH)/%.ipynb
- jupyter-nbconvert --to=pdf --output-dir=resources --output=$* --LatexExporter.template_file=resources/nbexport.tplx $^
-
-.PHONY: clean
-clean:
- rm -f ${main_tex}.aux ${main_tex}.bbl ${main_tex}.bcf ${main_tex}.log ${main_tex}.blg
- rm -f ${main_tex}.out ${main_tex}.run.xml texput.log
- rm -f ${brief_tex}.aux ${brief_tex}.bbl ${brief_tex}.bcf ${brief_tex}.log ${brief_tex}.blg
- rm -f ${brief_tex}.out ${brief_tex}.run.xml texput.log
-
diff --git a/doc/paper/circuits.ipynb b/doc/paper/circuits.ipynb
deleted file mode 100644
index 2e78b30..0000000
--- a/doc/paper/circuits.ipynb
+++ /dev/null
@@ -1,1115 +0,0 @@
-{
- "cells": [
- {
- "cell_type": "code",
- "execution_count": 1,
- "metadata": {},
- "outputs": [],
- "source": [
- "import schemdraw\n",
- "from schemdraw import elements as elm"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 123,
- "metadata": {},
- "outputs": [
- {
- "data": {
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- "<!DOCTYPE svg PUBLIC \"-//W3C//DTD SVG 1.1//EN\"\n",
- " \"http://www.w3.org/Graphics/SVG/1.1/DTD/svg11.dtd\">\n",
- "<!-- Created with matplotlib (https://matplotlib.org/) -->\n",
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- " <metadata>\n",
- " <rdf:RDF xmlns:cc=\"http://creativecommons.org/ns#\" xmlns:dc=\"http://purl.org/dc/elements/1.1/\" xmlns:rdf=\"http://www.w3.org/1999/02/22-rdf-syntax-ns#\">\n",
- " <cc:Work>\n",
- " <dc:type rdf:resource=\"http://purl.org/dc/dcmitype/StillImage\"/>\n",
- " <dc:date>2020-12-01T15:29:56.159415</dc:date>\n",
- " <dc:format>image/svg+xml</dc:format>\n",
- " <dc:creator>\n",
- " <cc:Agent>\n",
- " <dc:title>Matplotlib v3.3.3, https://matplotlib.org/</dc:title>\n",
- " </cc:Agent>\n",
- " </dc:creator>\n",
- " </cc:Work>\n",
- " </rdf:RDF>\n",
- " </metadata>\n",
- " <defs>\n",
- " <style type=\"text/css\">*{stroke-linecap:butt;stroke-linejoin:round;}</style>\n",
- " </defs>\n",
- " <g id=\"figure_1\">\n",
- " <g id=\"patch_1\">\n",
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- "text/plain": [
- "<__main__.DiodeOptocoupler at 0x7ff215993c70>"
- ]
- },
- "execution_count": 123,
- "metadata": {},
- "output_type": "execute_result"
- }
- ],
- "source": [
- "class DiodeOptocoupler(schemdraw.elements.compound.ElementCompound):\n",
- " def __init__(self, *args, **kwargs):\n",
- " unit = 1.5\n",
- " super().__init__(*args, unit=unit, **kwargs)\n",
- "\n",
- " box = kwargs.get('box', True)\n",
- " boxfill = kwargs.get('boxfill', False)\n",
- " bpad = kwargs.get('boxpad', .2)\n",
- " label1, label2 = kwargs.get('label1'), kwargs.get('label2')\n",
- " rev1, rev2 = kwargs.get('reverse1', False), kwargs.get('reverse2', False)\n",
- "\n",
- " D1 = self.add(elm.Diode(d='down', reverse=rev1))\n",
- " D2 = self.add(elm.Diode(d='down', reverse=rev2, at=[2, 0]))\n",
- " if label1:\n",
- " self.segments.append(schemdraw.segments.SegmentText(D1.start + (0, 0.5), label1))\n",
- " if label2:\n",
- " self.segments.append(schemdraw.segments.SegmentText(D2.start + (0, 0.5), label2))\n",
- " \n",
- " self.add(elm.Arrow('r', at=[.6, -unit/2 + .2], l=.4, headwidth=.15, headlength=.4))\n",
- " self.add(elm.Arrow('r', at=[.6, -unit/2 - .2], l=.4, headwidth=.15, headlength=.4))\n",
- "\n",
- " bbox = self.get_bbox()\n",
- " if box:\n",
- " self.add(elm.Rect(\n",
- " 'r', at=[0, 0],\n",
- " corner1=[bbox.xmin-bpad, bbox.ymin-bpad],\n",
- " corner2=[bbox.xmax+bpad, bbox.ymax+bpad],\n",
- " fill=boxfill, zorder=0))\n",
- "\n",
- " A = self.add(elm.Line('r', at=D2.start, l=bpad*2))\n",
- " B = self.add(elm.Line('r', at=D2.end, l=bpad*2))\n",
- " C = self.add(elm.Line('l', at=D1.start, tox=bbox.xmin-bpad))\n",
- " D = self.add(elm.Line('l', at=D1.end, tox=bbox.xmin-bpad))\n",
- " self.anchors['anode1'] = C.end\n",
- " self.anchors['cathode1'] = D.end\n",
- " self.anchors['anode2'] = B.end\n",
- " self.anchors['cathode2'] = A.end\n",
- "DiodeOptocoupler(box=False, reverse2=True, label2='D2')"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 177,
- "metadata": {},
- "outputs": [
- {
- "data": {
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diff --git a/doc/paper/concept_vis_one_axis.pdf b/doc/paper/concept_vis_one_axis.pdf
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diff --git a/doc/paper/goette_inertial_hsms_v1_5_eprint.pdf b/doc/paper/goette_inertial_hsms_v1_5_eprint.pdf
deleted file mode 100755
index 8fdb2b9..0000000
--- a/doc/paper/goette_inertial_hsms_v1_5_eprint.pdf
+++ /dev/null
Binary files differ
diff --git a/doc/paper/iacrtrans.cls b/doc/paper/iacrtrans.cls
deleted file mode 100755
index bf42a75..0000000
--- a/doc/paper/iacrtrans.cls
+++ /dev/null
@@ -1,448 +0,0 @@
-% IACR Transactions DOCUMENT CLASS -- version 0.24 (26 August 2016)
-% Written by Gaetan Leurent gaetan.leurent@inria.fr (2016)
-%
-% To the extent possible under law, the author(s) have dedicated all
-% copyright and related and neighboring rights to this software to the
-% public domain worldwide. This software is distributed without any
-% warranty.
-%
-% You should have received a copy of the CC0 Public Domain Dedication
-% along with this software. If not, see
-% <http://creativecommons.org/publicdomain/zero/1.0/>.
-%
-%
-%%% Class options:
-%
-% [preprint] Preprint (no copyright info)
-% [submission] Anonymous submission
-% [spthm] Emulate llncs sptheorem and remove automatic \qed in proof
-% [nohyperref] Disable automatic loading of hyperref
-% [draft]
-%
-%%% HOWTO use this class
-%
-%% Title
-% \title[short]{Long title}
-%
-%% Authors/affiliation:
-% \author{Alice \and Bob}
-% \institute{ABC\\ \email{alice@abc} \and DEF\\ \email{bob@def}}
-%
-%% Keywords/abstract:
-% \keywords{banana \and apple}
-% \begin{abstract}
-% Lorem ipsum dolor sit amet...
-% \end{abstract}
-%
-%% Warnings
-% - please don't use any \pagestyle of \thispagestyle command
-% - if you have proof with explicit \qed inside, you should either
-% remove \qed symbols, replace them by \qedhere, or add option [spthm]
-
-\NeedsTeXFormat{LaTeX2e}[1995/12/01]
-\ProvidesClass{iacrtrans}[2016/08/26 v0.24 IACR Transactions Author Class]
-
-% Common definitions
-\def\publname{IACR Transactions on Cryptographic Hardware and Embedded Systems}
-\def\IACR@vol{0}
-\def\IACR@no{0}
-\def\IACR@fp{1}
-\def\IACR@DOI{XXXXXXXX}
-\usepackage{lastpage}
-\def\IACR@lp{\pageref*{LastPage}}
-
-\newcommand{\setfirstpage}[1]{\def\IACR@fp{#1}\setcounter{page}{#1}}
-\newcommand{\setlastpage}[1]{\def\IACR@lp{#1}}
-\newcommand{\setvolume}[1]{\def\IACR@vol{#1}}
-\newcommand{\setnumber}[1]{\def\IACR@no{#1}}
-\newcommand{\setDOI}[1]{\def\IACR@DOI{#1}}
-
-% Options
-\newif\if@loadhr
-\@loadhrtrue
-\DeclareOption{nohyperref}{\@loadhrfalse}
-\newif\if@floatrow
-\@floatrowfalse
-\DeclareOption{floatrow}{\@floatrowtrue}
-\newif\if@submission
-\@submissionfalse
-\newif\if@preprint
-\@preprintfalse
-\DeclareOption{final}{\PassOptionsToClass{\CurrentOption}{article}} % Default
-\DeclareOption{preprint}{\@preprinttrue}
-\DeclareOption{submission}{\@submissiontrue}
-\DeclareOption{draft}{\@preprinttrue\PassOptionsToClass{\CurrentOption}{article}}
-\newif\if@spthm
-\@spthmfalse
-\DeclareOption{spthm}{\@spthmtrue}
-
-\DeclareOption*{\PassOptionsToClass{\CurrentOption}{article}}
-\ProcessOptions\relax
-
-% article class with a4paper
-\LoadClass[10pt,twoside]{article}[2007/10/19]
-
-% Geometry
-\RequirePackage[a4paper,hscale=0.65,vscale=0.75,marginratio=1:1]{geometry}
-
-% Title fonts: bf+sf
-\RequirePackage{sectsty}
-\allsectionsfont{\sffamily\boldmath}
-% Also for descrptions
-\renewcommand*\descriptionlabel[1]{\hspace\labelsep
- \normalfont\bfseries\sffamily #1}
-
-
-% Title/Author/affiliations
-\def\@institute{No institute given.}
-\newcommand{\institute}[1]{\gdef\@institute{#1}}
-\newcommand{\authorrunning}[1]{\gdef\IACR@runningauthors{#1}}
-\newcommand{\titlerunning}[1]{\gdef\IACR@runningtitle{#1}}
-
-\newcounter{IACR@author@cnt}
-\newcounter{IACR@inst@cnt}
-\newif\if@IACR@autoinst
-\@IACR@autoinsttrue
-\def\IACR@author@last{0}
-
-\renewcommand\maketitle{\par
- \begingroup
- \renewcommand\thefootnote{\@fnsymbol\c@footnote}%
- \long\def\@makefntext##1{\parindent 1em\noindent
- \hb@xt@1.8em{%
- \hss\@textsuperscript{\normalfont\@thefnmark}}##1}%
- \newpage
- \global\@topnum\z@ % Prevents figures from going at top of page.
- \@maketitle
- \thispagestyle{title}\@thanks
- \endgroup
- \setcounter{footnote}{0}%
- \global\let\thanks\relax
- \global\let\maketitle\relax
- \global\let\@maketitle\relax
- \global\let\@thanks\@empty
-% \global\let\@author\@empty
- \global\let\@date\@empty
-% \global\let\@title\@empty
- \global\let\title\relax
- \global\let\author\relax
- \global\let\date\relax
- \global\let\and\relax
-}
-\def\@maketitle{%
- % Count authors and affiliations
- \setcounter{IACR@author@cnt}{1}%
- \setcounter{IACR@inst@cnt}{1}%
- \setbox0\hbox{\def\thanks##1{\global\@IACR@autoinstfalse}\def\inst##1{\global\@IACR@autoinstfalse}\def\and{\stepcounter{IACR@author@cnt}}\@author}%
- \setbox0\hbox{\def\and{\stepcounter{IACR@inst@cnt}}\@institute}%
- \xdef\IACR@author@last{\theIACR@author@cnt}%
- \edef\IACR@inst@last{\theIACR@inst@cnt}%
- \ifnum\IACR@author@last=\IACR@inst@last\else\@IACR@autoinstfalse\fi
- \ifnum\IACR@author@last=1 \@IACR@autoinstfalse\fi
- \newpage
- \null
- \vskip 2em%
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index a24a7ec..0000000
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@@ -1,249 +0,0 @@
-% Encoding: UTF-8
-@comment{x-kbibtex-encoding=utf-8}
-
-@Book{anderson2020,
- author = {Ross Anderson},
- date = {2020-09-16},
- title = {Security Engineering},
- isbn = {978-1-119-64281-7},
-}
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-@techreport{smith1998,
- author = {Sean Smith and Steve Weingart},
- date = {1998-02-19},
- institution = {IBM T.J. Watson Research Center},
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-@Thesis{vrijaldenhoven2004,
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- institution = {Technische Universiteit Eindhoven},
- title = {Acoustical Physical Uncloneable Functions},
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- url = {https://pure.tue.nl/ws/files/46971492/600055-1.pdf},
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diff --git a/doc/paper/rotohsm_paper.pdf b/doc/paper/rotohsm_paper.pdf
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-\documentclass[nohyperref]{iacrtrans}
-\usepackage[T1]{fontenc}
-\usepackage[
- backend=biber,
- style=numeric,
- natbib=true,
- url=false,
- doi=true,
- eprint=false
- ]{biblatex}
-\addbibresource{rotohsm.bib}
-\usepackage{amssymb,amsmath}
-\usepackage{eurosym}
-\usepackage{wasysym}
-\usepackage{amsthm}
-
-\usepackage[binary-units]{siunitx}
-\DeclareSIUnit{\baud}{Bd}
-\DeclareSIUnit{\year}{a}
-\usepackage{commath}
-\usepackage{graphicx,color}
-\usepackage{subcaption}
-\usepackage{array}
-\usepackage{hyperref}
-
-\renewcommand{\floatpagefraction}{.8}
-\newcommand{\degree}{\ensuremath{^\circ}}
-\newcolumntype{P}[1]{>{\centering\arraybackslash}p{#1}}
-\newcommand{\partnum}[1]{\texttt{#1}}
-
-\begin{document}
-
-\title[Can't Touch This]{Inertial HSMs Thwart Advanced Physical Attacks}
-\author{Jan Sebastian Götte \and Björn Scheuermann}
-\institute{HIIG\\ \email{ihsm@jaseg.de} \and HU Berlin \\ \email{scheuermann@informatik.hu-berlin.de}}
-% FIXME keywords
-\keywords{hardware security \and implementation \and smart cards \and electronic commerce}
-\maketitle
-
-\begin{abstract}
- In this paper, we introduce a novel countermeasure against physical attacks: Inertial hardware security modules
- (iHSMs). Conventional systems have in common that their security requires the crafting of fine sensor structures
- that respond to minute manipulations of the monitored security boundary or volume. Our approach is novel in that we
- reduce the sensitivity requirement of security meshes and other sensors and increase the complexity of any
- manipulations by rotating the security mesh or sensor at high speed---thereby presenting a moving target to an
- attacker. Attempts to stop the rotation are easily monitored with commercial MEMS accelerometers and gyroscopes.
- Our approach leads to a HSM that can easily be built from off-the-shelf parts by any university electronics lab, yet
- offers a level of security that is comparable to commercial HSMs. We have built a proof of concept hardware
- prototype that demonstrates solutions to the concept's main engineering challenges. As part of this proof of
- concept, we have found that a system using a coarse security mesh made from commercial printed circuit boards and an
- automotive high g-force accelerometer already provides a useful level of security.
-\end{abstract}
-
-\section{Introduction}
-
-While information security technology has matured a great deal in the last half century, physical security not kept up
-with the pace of the remainder of this industry. Given the right skills, physical access to a computer still often
-allows full compromise. The physical security of modern server hardware hinges on what lock you put on the room it is
-in.
-
-Currently, servers and other computers are rarely physically secured as a whole. Servers sometimes have a simple lid
-switch and are put in locked ``cages'' inside guarded facilities. This usually provides a good compromise between
-physical security and ease of maintenance. To handle highly sensitive data in applications such as banking or public key
-infrastructure, general-purpose and low-security servers are augmented with dedicated, physically secure cryptographic
-co-processors such as trusted platform modules (TPMs) or hardware security modules (HSMs). Using a limited amount of
-trust in components such as the CPU, the larger system's security can then be reduced to that of its physically secured
-TPM~\cite{newman2020,frazelle2019,johnson2018}.
-Like smartcards, TPMs rely on a modern IC being hard to tamper with. Shrinking things to the nanoscopic level to secure
-them against tampering is a good engineering solution for some years to come. However, in essence this is a type of
-security by obscurity: Obscurity here referring to the rarity of the equipment necessary to attack modern
-ICs~\cite{albartus2020,anderson2020}.
-
-In contrast to TPMs and Smartcards, HSMs rely on an active security barrier usually consisting of a fragile foil with
-conductive traces. These traces are much larger scale than a smart card IC's microscopic structures, and instead are
-designed to be very hard to remove intact. While we are certain that there still are many insights to be gained in both
-technologies, we wish to introduce a novel approach to sidestep the manufacturing issues of both and provide radically
-better security against physical attacks. Our core observation is that any cheap but coarse HSM technology can be made
-much more difficult to attack by moving it very quickly.
-
-For example, consider an HSM as it is used in online credit card payment processing. Its physical security level is set
-by the structure size of its security mesh. An attack on its mesh might involve fine drill bits, needles, wires, glue,
-solder and lasers~\cite{drimer2008}. Now consider the same HSM mounted on a large flywheel. In addition to its usual
-defenses, this modified HSM is now equipped with an accelerometer that it uses to verify that it is spinning at high
-speed. How would an attacker approach this HSM? They would have to either slow down the rotation---which triggers the
-accelerometer's monitoring circuit---or they would have to attack the HSM in motion. The HSM literally becomes a moving
-target. At slow speeds, rotating the entire attack workbench might be possible---but rotating frames of reference
-quickly become inhospitable to human life (see Section~\ref{sec_swivel_chair_attack}). Since non-contact electromagnetic
-or optical attacks are more limited in the first place and can be shielded, we have effectively forced the attacker to
-use an ``attack robot''.
-
-This paper contains the following contributions:
-\begin{enumerate}
- \item We present the \emph{Inertial HSM} concept. Inertial HSMs enable cost effective, small scale production of
- highly secure HSMs.
- \item We discuss possible tamper sensors for inertial HSMs.
- \item We explore the design space of our inertial HSM concept.
- \item We present our work on a prototype inertial HSM (Figure~\ref{prototype_picture}).
- \item We present an analysis on the viability of using commodity MEMS accelerometers as braking sensors.
- % FIXME \item Measurement of the prototype HSM's susceptibility to various types of attack.
-\end{enumerate}
-
-\begin{figure}
- \center
- \includegraphics[width=12cm]{prototype_pic2.jpg}
- \caption{The protoype as we used it to test power transfer and bidirectional communication between stator and rotor.
- This picture shows the proof of concept prototype's configuration that we used for accelerometer characterization
- (Section~\ref{sec_accel_meas}) without the vertical security mesh struts that connect the circular top and bottom
- outer meshes.}
- \label{prototype_picture}
-\end{figure}
-
-In Section~\ref{sec_related_work}, we will give an overview of the state of the art in HSM physical security. On this
-basis, in Section~\ref{sec_ihsm_construction} we will elaborate the principles of our Inertial HSM approach. We will
-analyze its weaknesses in Section~\ref{sec_attacks}. Based on these results we have built a proof of concept hardware
-prototype that whose design we will elaborate in Section~\ref{sec_proto}. In Section~\ref{sec_accel_meas} we present our
-characterization of an automotive MEMS accelerometer IC as a rotation sensor in this proof of concept prototype. We
-conclude this paper with a general evaluation of our design in Section~\ref{sec_conclusion}.
-
-\section{Related work}
-\label{sec_related_work}
-% summaries of research papers on HSMs. I have not found any actual prior art on anything involving mechanical motion
-% beyond ultrasound.
-
-In this section, we will briefly explore the history of HSMs and the state of academic research on active tamper
-detection.
-
-HSMs are an old technology that traces back decades in its electronic realization. Today's common approach of monitoring
-meandering electrical traces on a fragile foil that is wrapped around the HSM essentially transforms the security
-problem into the challenge to manufacture very fine electrical traces on a flexible foil~\cite{isaacs2013, immler2019,
-anderson2020}. There has been some research on monitoring the HSM's inside using e.g.\ electromagnetic
-radiation~\cite{tobisch2020, kreft2012} or ultrasound~\cite{vrijaldenhoven2004} but none of this research has found
-widespread adoption yet.
-
-HSMs can be compared to physical seals~\cite{anderson2020}. Both are tamper evident devices. The difference is that a
-HSM continuously monitors itself whereas a physical seal only serves to record tampering and requires someone to examine
-it. This examination can be by eye in the field, but it can also be carried out in a laboratory using complex equipment.
-An HSM in principle has to have this examination equipment built-in.
-
-Physical seals are used in a wide variety of applications, but the most interesting ones from a research point of view
-that are recorded in public literature are those used in monitoring of nuclear material under the International Atomic
-Energy Authority (IAEA). Most of these seals use the same approach that is used in Physically
-Uncloneable Functions (PUFs), though their development predates that of PUFs by several decades. The seal is created in
-a way that intentionally causes large, random device to device variations. These variations are precisely recorded at
-deployment. At the end of the seal's lifetime, the seal is returned from the field to the lab and closely examined to
-check for any deviations from the seal's prior recorded state. The type of variation used in these seals includes random
-scratches in metal parts and random blobs of solder (IAEA metal cap seal), randomly cut optical fibers (COBRA seal), the
-uncontrollably random distribution of glitter particles in a polymer matrix (COBRA seal prototypes) as well as the
-precise three-dimensional surface structure of metal parts at microscopic scales (LMCV)~\cite{iaea2011}.
-
-The IAEA's equipment portfolio does include electronic seals such as the EOSS. These devices are intended for remote
-reading, similar to an HSM. They are constructed from two components: A cable that is surveilled for tampering, and a
-monitoring device. The monitoring device itself is in effect an HSM and uses a security mesh foil such as it is used in
-commercial HSMs.
-
-In~\cite{anderson2020}, Anderson gives a comprehensive overview on physical security. An example HSM that they cite is
-the IBM 4758 HSM whose details are laid out in depth in~\cite{smith1998}. This HSM is an example of an industry-standard
-construction. Although its turn of the century design is now a bit dated, the construction techniques of the physical
-security mechanisms have not evolved much in the last two decades. Besides some auxiliary temperature and radiation
-sensors to guard against attacks on the built-in SRAM memory, the module's main security barrier uses the traditional
-construction of a flexible mesh foil wrapped around the module's core. In~\cite{smith1998}, the authors state that the
-module monitors this mesh for short circuits, open circuits and conductivity. The fundamental approach to tamper
-detection and construction is similar to other commercial
-offerings~\cite{obermaier2018,drimer2008,anderson2020,isaacs2013}.
-
-Shifting our focus from industry use to the academic state of the art, in~\cite{immler2019}, Immler et al. describe an
-HSM based on precise capacitance measurements of a security mesh, creating a PUF from the mesh. In contrast to
-traditional meshes, the mesh they use consists of a large number of individual traces (more than 30 in their example).
-Their concept promises a very high degree of protection. The main disadvantages of their concept are a limitation in
-covered area and component height, as well as the high cost of the advanced analog circuitry required for monitoring. A
-core component of their design is that they propose its use as a PUF to allow for protection even when powered off,
-similar to a smart card---but the design is not limited to this use.
-
-In~\cite{tobisch2020}, Tobisch et al.\ describe a construction technique for a hardware security module that is based
-around commodity WiFi hardware inside a conductive enclosure. In their design, an RF transmitter transmits a reference
-signal into the RF cavity formed by the conductive enclosure. One or more receivers listen for the signal's reflections
-and use them to characterize the RF cavity w.r.t.\ phase and frequency response. Their fundamental assumption is that
-the RF behavior of the cavity is inscrutable from the outside, and that even a small disturbance anywhere within the
-volume of the cavity will cause a significant change in its RF response. A core component of the work of Tobisch et
-al.~\cite{tobisch2020}\ is that they use commodity WiFi hardware to reduce the cost of the HSM's sensing circuitry. The
-resulting system is likely both much cheaper and capable of protecting a much larger security envelope than designs
-using finely patterned foil security meshes such as~\cite{immler2019}, at the cost of worse and less predictable
-security guarantees. Where~\cite{tobisch2020} use electromagnetic radiation, Vrijaldenhoven
-in~\cite{vrijaldenhoven2004} uses ultrasound waves travelling on a surface acoustic wave (SAW) device to a similar end.
-
-While Tobisch et al.~\cite{tobisch2020}\ approach the sensing frontend cost as their primary optimization target, the
-prior work of Kreft and Adi~\cite{kreft2012} considers sensing quality. Their target is an HSM that envelopes a volume
-barely larger than a single chip. They theorize how an array of distributed RF transceivers can measure the physical
-properties of a potting compound that has been loaded with RF-reflective grains. In their concept, the RF response
-characterized by these transceivers is shaped by the precise three-dimensional distribution of RF-reflective grains
-within the potting compound.
-
-To the best of our knowledge, we are the the first to propose a mechanically moving HSM security barrier as part of a
-hardware security module. Most academic research concentrates on the issue of creating new, more sensitive security
-barriers for HSMs~\cite{immler2019} while commercial vendors concentrate on means to certify and cheaply manufacture
-these security barriers~\cite{drimer2008}. Our concept instead focuses on the issue of taking any existing, cheap
-low performance security barrier and transforming it into a marginally more expensive but high performance one. The
-closest to a mechanical HSM that we were able to find during our research is an 1988 patent~\cite{rahman1988} that
-describes a mechanism to detect tampering along a communication cable by enclosing the cable inside a conduit filled
-with pressurized gas.
-
-\subsection{Patent literature}
-During development, we performed several hours of research on prior art for the inertial HSM concept. Yet, we could not
-find any mentions of similar concepts either in academic literature or in patents. Thus, while we cannot give any
-guarantees, we seem likely to be the inventors of this idea and we are fairly sure it is not covered by any patents or
-other restrictions at this point in time.
-
-Since the concept is primarily attractive for small-scale production and since cheaper mass-production alternatives are
-already commercially available, we have decided against applying for a patent and we wish to make it available to the
-general public without any restrictions on its use. We invite you build on our work as you wish and to base your own
-work on our publications without any fees or commercial restrictions. Where possible, we ask you to cite this paper and
-attribute the inertial HSM concept to its authors.
-
-\section{Inertial HSM construction and operation}
-\label{sec_ihsm_construction}
-
-Mechanical motion has been proposed as a means of making things harder to see with the human eye~\cite{haines2006} and
-is routinely used in military applications to make things harder to hit~\cite{terdiman2013} but we seem to be the first
-to use it in tamper detection.
-
-The core questions in the design of an inertial HSM are the following:
-
-\begin{enumerate}
- \item What \textbf{type of motion} to use, such as rotation, pendulum motion, or linear motion.
- \item How to construct the \textbf{tamper detection sensor}.
- \item How to \textbf{detect braking} of the IHSM's movement.
- \item The \textbf{mechanical layout} of the system.
-\end{enumerate}
-
-We will approach these questions one by one in the following subsections.
-
-\subsection{Inertial HSM motion}
-\label{sec_ihsm_motion}
-
-First, there are several ways that we can approach motion. There is periodic, aperiodic and continuous motion. There is
-also linear motion as well as rotation. We can also vary the degree of electronic control in this motion. The main
-constraints we have on the HSM's motion pattern are that it needs to be (almost) continuous so as to not expose any weak
-spots during instantaneous standstill of the HSM. Additionally, for space efficiency the HSM has to stay within a
-confined space. This means that linear motion would have to be periodic, like that of a pendulum. Such periodic linear
-motion will have to quickly reverse direction at its apex so the device is not stationary long enough for this to become
-a weak spot.
-
-In contrast to linear motion, rotation is space-efficient and can be continuous if the axis of rotation is inside the
-device. In case it has a fixed axis, rotation will expose a weak spot at the axis of rotation where the surface's
-tangential velocity is low. Faster rotation can lessen the security impact of this fact at the expense of power
-consumption and mechanical stress, but it can never eliminate it. This effect can be alleviated in two ways: Either by
-adding additional tamper protection at the axis, or by having the HSM perform a compound rotation that has no fixed
-axis.
-
-Large centrifugal acceleration at high speeds poses the engineering challenge of preventing rapid unscheduled
-disassembly of the device, but it also creates an obstacle to any attacker trying to manipulate the device in what we
-call a \emph{swivel chair attack} (see Section~\ref{sec_swivel_chair_attack}). An attacker trying to follow the motion
-would have to rotate around the same axis. By choosing a suitable rotation frequency we can prevent an attacker from
-following the devices motion since doing so would subject them to impractically large centrifugal forces. Essentially,
-this limits the approximate maximum size and mass of an attacker based on an assumption on tolerable centrifugal force.
-
-In this paper we focus on rotating IHSMs for simplicity of construction. For our initial research, we are focusing on
-systems that have a fixed axis of rotation due to their simple construction but we do wish to note the challenge of
-hardening the shaft against tampering that any production device would have to tackle.
-
-\subsection{Tamper detection mesh construction}
-
-Once we have decided how our IHSM's security barrier should move, what remains is the actual implementation
-of that security barrier. There are two movements that we have observed that are key to our work. On the one hand, there
-is the widespread industry use of delicate tamper sensing mesh membranes. The usage of such membranes in systems
-deployed in the field for a variety of use cases from low security payment processing devices to high security
-certificate management at a minimum tells us that a properly implemented mesh \emph{can} provide a practical level of
-security. On the other hand, in contrast to this industry focus, academic research has largely focused on ways to
-fabricate enclosures that embed characteristics of a Physically Uncloneable Function. By using stochastic properties of
-the enclosure material to form a PUF, such academic designs effectively leverage signal processing techniques to improve
-the system's security level by a significant margin.
-
-In our research, we focus on security meshes as our IHSM's tamper sensors. Most of the cost in commercial security mesh
-implementations lies in the advanced manufacturing techniques and special materials necessary to achieve a sensitive
-mesh at fine structure sizes. The foundation of an IHSM security is that by moving the mesh even a primitive, coarse
-mesh made e.g.\ from mesh traces on a PCB becomes very hard to attack in practice. This allows us to use a simple
-construction made up from low-cost components. Additionally, the use of a mesh allows us to only spin the mesh itself
-and its monitoring circuit and keep the payload inside the mesh stationary. Tamper sensing technologies that use the
-entire volume of the HSM such as RF-based systems do not allow for this degree of freedom in their design: They would
-require the entire IHSM to spin, including its payload, which would entail costly and complex systems for data and power
-transfer from the outside to the payload.
-
-\subsection{Braking detection}
-
-The security mesh is a critical component in the IHSM's defense against physical attacks, but its monitoring is only one
-half of this defense. The other half consists of a reliable and sensitive braking detection system. This system must be
-able to quickly detect any slowing of the IHSM's rotation. Ideally, a sufficiently sensitive sensor should be able to
-measure any external force applied to the IHSM's rotor and should already trigger a response at the first signs of a
-manipulation attempt.
-
-While the obvious choice to monitor rotation would be a tachometer such as a magnetic or opitical sensor attached to the
-IHSM's shaft, this would be a poor choice in our application. Both optical and magnetic sensors are susceptible to
-contact-less interference from outside. A different option would be to use feedback from the motor driver electronics.
-When using a BLDC motor, the driver electronics precisely know the rotor's position at all times. The issue with this
-approach is that depending on construction, it might invite attacks at the mechanical interface between mesh and the
-motor's shaft. If an attacker can decouple the mesh from the motor e.g.\ by drilling, laser ablation or electrical
-discharge machining (EDM) on the motor's shaft, the motor could keep spinning at its nominal frequency while the mesh is
-already standing still.
-
-Instead of a stator-side sensor like a magnetic tachometer or feedback from the BLDC controller, an accelerometer placed
-inside the spinning mesh monitoring circuit would be a good component to serve as an IHSM's tamper sensor. Modern, fully
-intergrated MEMS accelerometers are very precise. By comparing acceleration measurements against a model of the device's
-mechanical motion, deviations can quickly be detected. This limits an attacker's ability to tamper with the device's
-motion. It may also allow remote monitoring of the device's mechanical components such as bearings: MEMS accelerometers
-are fast enough to capture vibrations, which can be used as an early warning sign of failing mechanical
-components~\cite{kvk2019,sh2016,adc2019,e2013}.
-
-In a spinning IHSM, an accelerometer mounted at a known radius with its axis pointing radially will measure centrifugal
-acceleration. Centrifugal acceleration rises linearly with radius, and with the square of frequency: $a=\omega^2 r$. For
-a given target speed of rotation, the accelerometer's location has to be carefully chosen to maximize dynamic range. A
-key point here is that for rotation speeds between $500$ and $\SI{1000}{rpm}$, centrifugal acceleration already becomes
-very large at a radius of just a few $\si{\centi\meter}$. At $\SI{1000}{rpm}\approx\SI{17}{\hertz}$ at a
-$\SI{10}{\centi\meter}$ radius acceleration already is above $\SI{1000}{\meter\per\second}$ or $100\,g$. While
-beneficial for security, this large acceleration leads to two practical constraints. First, off-axis performance of
-commercial accelerometers is usually in the order of $\SI{1}{\percent}$ so this large acceleration will feed through
-into all accelerometer axes, even those that are tangential to the rotation. Second, we either have to place the
-accelerometer close to the axis or we are limited to a small selection of high-$g$ accelerometers mostly used in
-automotive applications.
-
-To evaluate the feasibility of accelerometers as tamper sensors we can use a simple benchmark: Let us assume that an
-IHSM is spinning at $\SI{1000}{rpm}$ and that we wish to detect any attempt to brake it below $\SI{500}{rpm}$. The
-difference in centrifugal acceleration that our accelerometer will have to detect then is a factor of
-$\frac{\omega_2^2}{\omega_1^2}=4$. If we choose our accelerometer's location to maximize its dynamic range, any
-commercial MEMS accelerometer should suffice for this degree of accuracy even over long timespans. For rapid
-deceleration, commercial accelerometers will be much more sensitive as effects of long-term drift can be ignored. If we
-wish to also detect very slow deceleration, we have to take into account the accelerometer's drift characteristics.
-
-In Section~\ref{sec_accel_meas} below we conduct an empirical evaluation of a commercial automotive high-$g$ MEMS
-accelerometer for braking detection in our prototype IHSM.
-
-\subsection{Mechanical layout}
-
-With our IHSM's components taken care of, what remains to be decided is how to put together these individual components
-into a complete device. A basic spinning HSM might look like shown in Figure~\ref{fig_schema_one_axis}. Shown are the
-axis of rotation, an accelerometer on the rotating part that is used to detect braking, the protected payload and the
-area covered by the rotating tamper detection mesh. A key observation is that we only have to move the tamper
-protection mesh, not the entire contents of the HSM. The HSM's payload and with it most of the HSM's mass can be
-stationary. This reduces the moment of inertia of the moving part. This basic schema accepts a weak spot at the point
-where the shaft penetrates the spinning mesh. This trade-off makes for a simple mechanical construction and allows
-power and data connections to the stationary payload through a hollow shaft.
-
-\begin{figure}
- \center
- \includegraphics{concept_vis_one_axis.pdf}
- \caption{Concept of a simple spinning Inertial HSM. 1 - Shaft. 2 - Security mesh. 3 - Payload. 4 -
- Accelerometer. 5 - Shaft penetrating security mesh.}
- \label{fig_schema_one_axis}
-\end{figure}
-
-The spinning mesh must be designed to cover the entire surface of the payload, but it suffices if it sweeps over every
-part of the payload once per rotation. This means we can design longitudinal gaps into the mesh that allow outside air
-to flow through to the payload. In traditional boundary-sensing HSMs, cooling of the payload processor is a serious
-issue since any air duct or heat pipe would have to penetrate the HSM's security boundary. This problem can only be
-solved with complex and costly siphon-style constructions, so in commercial systems heat conduction is used
-exclusively~\cite{isaacs2013}. This limits the maximum power dissipation of the payload and thus its processing power.
-Using longitudinal gaps in the mesh, our setup allows direct air cooling of regular heatsinks. This unlocks much more
-powerful processing capabilities that greatly increase the maximum possible power dissipation of the payload. In an
-evolution of our design, the spinning mesh could even be designed to \emph{be} a cooling fan.
-
-\section{Attacks}
-\label{sec_attacks}
-
-After outlining the basic mechanical design of an inertial HSM above, in this section we will detail possible ways to
-attack it. At the core of an IHSM's defenses is the same security mesh or other technology as it is used in traditional
-HSMs. This means that in the end an attacker will have to perform the same steps they would have to perform to attack a
-traditional HSM. Only, they will either have to perform these attack steps with a tool that follows the HSMs rotation
-at high speed or they will first have to defeat the braking sensor. Attacking the IHSM in motion may require specialized
-mechanical tools, CNC actuators or even a contactless attack using a laser, plasma jet or water jet.
-
-\subsection{The Swivel Chair Attack}
-\label{sec_swivel_chair_attack}
-
-First we will consider the most basic of all attacks: A human attacker holding a soldering iron trying to rotate
-themselves along with the mesh using a very fast swivel chair. Let us pessimistically assume that this co-rotating
-attacker has their center of mass on the axis of rotation. The attacker's body is likely on the order of
-$\SI{200}{\milli\meter}$ wide along its shortest axis, resulting in a minimum radius from axis of rotation to surface of
-about $\SI{100}{\milli\meter}$. Wikipedia lists horizontal g forces in the order of $\SI{20}{g}$ as the upper end of the
-range tolerable by humans for seconds at a time or longer. We thus set our target acceleration to
-$\SI{100}{g}\;\approx\;\SI{1000}{\meter\per\second^2}$, a safety factor of $5$ past that range. Centrifugal
-acceleration is $a=\omega^2 r$. In our example this results in a minimum angular velocity of $f_\text{min} =
-\frac{1}{2\pi}\sqrt{\frac{a}{r}} = \frac{1}{2\pi}\sqrt{\frac{\SI{1000}{\meter\per\second^2}}{\SI{100}{\milli\meter}}}
-\approx \SI{16}{\hertz} \approx \SI{1000}{rpm}$. From this we can conclude that even at moderate speeds of
-$\SI{1000}{rpm}$ and above, a manual attack is no longer possible and any attack would have to be carried out using some
-kind of mechanical tool.
-
-\subsection{Mechanical weak spots}
-
-The tamper defense of an IHSM rests on the security mesh moving too fast to tamper. Depending on the type of motion
-used, the meshes speed may vary by location and over time. Our example configuration of a rotating mesh can keep moving
-continuously, so it does not have any time-dependent weak spots. It does however have a weak spot at its axis of
-rotation, at the point where the shaft penetrates the mesh. The meshes tangential velocity decreases close to the shaft,
-and the shaft itself may allow an attacker to insert tools such as probes into the device through the opening it
-creates. This issue is related to the issue conventional HSMs also face with their power and data connections. In
-conventional HSMs, power and data are routed into the enclosure through the PCB or flat flex cables sandwiched in
-between security mesh foil layers. In traditional HSMs this interface rarely is a mechanical weak spot since they use a
-thin mesh substrate and create a meandering path by folding the interconnect substrate/security mesh layers several
-times. In inertial HSMs, careful engineering is necessary to achieve the same effect. Figure~\ref{shaft_cm} shows
-variations of the shaft interface with increasing complexity.
-
-\begin{figure}
- \begin{subfigure}[t]{0.3\textwidth}
- \center
- \includegraphics[width=4cm]{ihsm_shaft_countermeasures_a.pdf}
- \caption{Cross-sectional view of the basic configuration with no special protection of the shaft. Red: Moving
- mesh -- Black: Stationary part.}
- \label{shaft_cm_a}
- \end{subfigure}
- \hfill
- \begin{subfigure}[t]{0.3\textwidth}
- \center
- \includegraphics[width=4cm]{ihsm_shaft_countermeasures_b.pdf}
- \caption{An internal counter-rotating disc greatly decreases the space available to attackers at the expense of
- another moving part and a second moving monitoring circuit.}
- \label{shaft_cm_a}
- \end{subfigure}
- \hfill
- \begin{subfigure}[t]{0.3\textwidth}
- \center
- \includegraphics[width=4cm]{ihsm_shaft_countermeasures_c.pdf}
- \caption{A second moving tamper detection mesh also enables more complex topographies.}
- \label{shaft_cm_a}
- \end{subfigure}
- \caption{Mechanical countermeasures to attacks through or close to the shaft of a fixed-axis rotating IHSM.}
- \label{shaft_cm}
-\end{figure}
-
-\subsection{Attacking the mesh in motion}
-
-To disable the mesh itself, an attacker can choose two paths. One is to attack the mesh itself, for example by bridging
-its traces. The other option is to tamper with the monitoring circuit to prevent a damaged mesh from triggering an
-alarm~\cite{dexter2015}. Attacks in both locations are electronic attacks, i.e.\ they require electrical contact to
-parts of the circuit. Traditionally, this contact is made by soldering a wire or by placing a probe such as a thin
-needle. We consider this type of attack hard to perform on an object spinning at high speed. Possible remaining attack
-avenues may be to rotate an attack tool in sync with the mesh, or to use a laser or ion beam fired at the mesh to cut
-traces or carbonize parts of the substrate to create electrical connections. Encapsulating the mesh in a potting
-compound and shielding it with a metal enclosure as is common in traditional HSMs will significantly increase the
-complexity of such attacks.
-
-\subsection{Attacks on the rotation sensor}
-
-Instead of attacking the mesh in motion, an attacker may also try to first stop the rotor. To succeed, they would need
-to falsify the rotor's MEMS accelerometer measurements. We can disregard electronic attacks on the sensor or the
-monitoring microcontroller because they would be no easier than attacking the mesh traces. What remains would be
-physical attacks of the accelerometer's sensing mechanism.
-MEMS accelerometers usually use a cantilever design in which a proof mass moves a cantilever whose precise position is
-measured electronically. A topic of recent academic interest have been acoustic attacks tampering with these
-mechanics~\cite{trippel2017}, but such attacks do not yield sufficient control to precisely falsify sensor readings.
-A possible more invasive attack may be to first decapsulate the sensor MEMS using laser ablation synchronized with the
-device's rotation. Then, a fast-setting glue such as a cyanoacrylate could be deposited on the MEMS, locking the
-mechanism in place. This type of attack can be mitigated by mounting the accelerometer in a shielded location inside the
-security envelope and by varying the rate of rotation over time.
-
-\subsection{Attacks on the alarm circuit}
-
-Besides trying to deactivate the tamper detection mesh, an electronic attack could also target the alarm circuitry
-inside the stationary payload, or the communication link between rotor and payload. The link can be secured using a
-cryptographically secured protocol like one would use for wireless radio links along with a high-frequency heartbeat
-message. The alarm circuitry has to be designed such that it is entirely contained within the HSM's security envelope.
-Like in conventional HSMs, it has to be built to either tolerate or detect environmental attacks using sensors for
-temperature, ionizing radiation, laser radiation, supply voltage variations, ultrasound or other vibration and gases or
-liquids. If a wireless link is used between the IHSM's rotor and stator, this link must be cryptographically secured.
-To prevent replay attacks link latency must continuously be measured, so this link must be bidirectional.
-% If it were unidirectional, an attacker could
-% act as a Man-in-the-Middle and replay the mesh's authenticated ``no alarm'' signal at slightly below real-time speed
-% (say at $\SI{99}{\percent}$ speed). The receiver would not be able to distinguish between this attack and ordinary
-% deviations in the transmitter's local clock frequency. Thus, after some time the attacker can simply stop the rotor and
-% break the mesh while replaying the leftover recorded ``no alarm'' signal. Given the frequency stability of commercial
-% crystals, this would yield the attacker several seconds of undisturbed attack time per hour of recording time.
-
-\subsection{Fast and violent attacks}
-
-A variation of the above attacks on the alarm circuitry is to simply destroy the part of the HSM that erases data in
-response to tampering before it can perform its job using a tool such as a large hammer or a gun. To mitigate this type
-of attack, the HSM must be engineered to be either tough or brittle: Tough enough that the tamper response circuitry
-will reliably withstand any attack for long enough to carry out its function or brittle in a way that during any attack,
-the payload is reliably destroyed before the tamper response circuitry.
-
-\section{Proof of Concept Prototype implementation}
-\label{sec_proto}
-
-As we elaborated above, the mechanical component of an IHSM significantly increases the complexity of any attack even
-when implemented using only common, off-the-shelf parts. In view of this amplification of design security we have
-decided to validate our theoretical studies by implementing a proof of concept prototype IHSM
-(Figure~\ref{prototype_picture}). The main engineering challenges we set out to solve in this proof of concept prototype
-were:
-
-\begin{enumerate}
- \item A mechanical design suitable for rapid prototyping that can withstand at least $\SI{500}{rpm}$.
- \item The Automatic generation of security mesh PCB layouts for quick adaption to new form factors.
- \item Non-contact power transmission from stator to rotor.
- \item Non-contact bidirectional data communication between stator and rotor.
-\end{enumerate}
-
-We will outline our findings on these challenges one by one in the following paragraphs.
-
-\subsection{Mechanical design}
-
-We sized our proof of concept prototype to have sufficient payload space for up to two full-size Raspberry Pi boards to
-approximate a traditional HSM's processing capabilities. We use printed circuit boards as the main structural material
-for the rotating part, and 2020 aluminium extrusion for its mounting frame. Figure~\ref{fig_proto_mesh} shows the
-rotor's mechanical PCB designs. The design uses a $\SI{6}{\milli\meter}$ brass tube as its shaft, which is already
-sufficiently narrow to pose a challenge to an attacker. The rotor is driven by a small hobby quadcopter motor. Our
-prototype incorporates a functional PCB security mesh. As we observed previously, this mesh only needs to cover every
-part of the system once per revolution, so we designed the longituninal PCBs as narrow strips to save weight.
-
-\subsection{PCB security mesh generation}
-
-% FIXME censor link in peer-review version!
-Our proof-of-concept security mesh covers a total of five interlocking mesh PCBs (Figure~\ref{mesh_gen_sample}). A sixth
-PCB contains the monitoring circuit and connects to these mesh PCBs. To speed up design iterations, we automated the
-generation of this security mesh through a plugin for the KiCAD EDA
-suite\footnote{\url{https://blog.jaseg.de/posts/kicad-mesh-plugin/}}. Figure~\ref{mesh_gen_viz} visualizes the mesh
-generation process. First, the target area is overlaid with a grid. Then, the algorithm produces a randomized tree
-covering the grid. Finally, individual mesh traces are traced according to a depth-first search through this tree.
-We consider the quality of the plugin's output sufficient for practical applications. Together with FreeCAD's KiCAD
-StepUp plugin, this results in an efficient toolchain from mechanical CAD design to production-ready PCB files.
-
-\begin{figure}
- \begin{subfigure}{0.35\textwidth}
- \center
- \includegraphics[height=7cm]{proto_3d_design.jpg}
- \caption{The 3D CAD design of the proof of concept prototype.}
- \end{subfigure}
- \hfill
- \begin{subfigure}{0.6\textwidth}
- \includegraphics[width=8cm]{rotor_stator.jpg}
- \center
- \caption{Assembled mechanical prototype rotor (left) and stator (right) PCB components.}
- \end{subfigure}
- \caption{Our proof of concept prototype IHSM's PCB security mesh design}
- \label{fig_proto_mesh}
-\end{figure}
-
-\begin{figure}
- \begin{subfigure}{\textwidth}
- \center
- \includegraphics[width=9cm]{mesh_gen_viz.pdf}
- \caption{Overview of the automatic security mesh generation process. 1 - Example target area. 2 - Grid overlay.
- 3 - Grid cells outside of the target area are removed. 4 - A random tree covering the remaining cells is
- generated. 5 - The mesh traces are traced along a depth-first walk of the tree. 6 - Result.}
- \label{mesh_gen_viz}
- \end{subfigure}
- \begin{subfigure}{\textwidth}
- \center
- \includegraphics[width=6cm]{mesh_scan_crop.jpg}
- \caption{Detail of a PCB produced with a generated mesh.}
- \label{mesh_gen_sample}
- \end{subfigure}
- \caption{Our automatic security mesh generation process}
- \label{mesh_gen_fig}
-\end{figure}
-
-\subsection{Power transmission from stator to rotor}
-
-The spinning mesh has its own autonomous monitoring circuit. This spinning monitoring circuit needs both power and data
-connectivity to the stator. To design the power link, we first have to estimate the monitoring circuit's power
-consumption. We base our calculation on the (conservative) assumption that the spinning mesh sensor should send its
-tamper status to the static monitoring circuit at least once every $T_\text{tx} = \SI{10}{\milli\second}$. At
-$\SI{100}{\kilo\baud}$, a transmission of a one-byte message in standard UART framing would take
-$\SI{100}{\micro\second}$ and yield an $\SI{1}{\percent}$ duty cycle. If we assume an optical or RF transmitter that
-requires $\SI{10}{\milli\ampere}$ of active current, this yields an average operating current of
-$\SI{100}{\micro\ampere}$. Reserving another $\SI{100}{\micro\ampere}$ for the monitoring circuit itself we arrive at an
-energy consumption of $\SI{1.7}{\ampere\hour}$ per year.
-
-This annual energy consumption is close to the capacity of a single CR123A lithium primary cell. Thus, by either using
-several such cells or by optimizing power consumption several years of battery life could easily be reached. In our
-proof of concept prototype we decided against using a battery to reduce rotor mass and balancing issues.
-
-We also decided against mechanically complex solutions such as slip rings or electronically complex ones such as
-inductive power transfer. Instead, we chose a simple setup consisting of a stationary lamp pointing at several solar
-cells on the rotor. At the monitoring circuit's low power consumption power transfer efficiency is irrelevant, so this
-solution is practical. Our system uses six series-connected solar cells mounted on the end of the cylindrical rotor
-that are fed into a large $\SI{33}{\micro\farad}$ ceramic buffer capacitor through a Schottky diode. This solution
-provides around $\SI{3.0}{\volt}$ at several tens of $\si{\milli\ampere}$ to the payload when illuminated using either
-a $\SI{60}{\watt}$ incandescent light bulb or a flicker-free LED studio light of similar brightness\footnote{LED lights
-intended for room lighting exhibit significant flicker that can cause the monitoring circuit to reset. Incandescent
-lighting requires some care in shielding the data link from the light bulb's considerable infrared output.}.
-
-\subsection{Data transmission between stator and rotor}
-
-Besides power transfer from stator to rotor, we need a reliable, bidirectional data link to transmit mesh status and a
-low-latency heartbeat signal. We chose to transport an $\SI{115}{\kilo\baud}$ UART signal through a simple IR link for a
-quick and robust solution. The link's transmitter directly drives a standard narrow viewing angle IR led through a
-transistor. The receiver has an IR PIN photodiode reverse-biased at $\frac{1}{2}V_\text{CC}$ feeding into an
-\texttt{MCP6494} general purpose opamp configured as an $\SI{100}{\kilo\ohm}$ transimpedance amplifier. As shown in
-Figure \ref{photolink_schematic}, the output of this TIA is amplified one more time before being squared up by a
-comparator. Our design trades off stator-side power consumption for a reduction in rotor-side power consumption by
-using a narrow-angle IR led and photodiode on the rotor, and wide-angle components at a higher LED current on the
-stator. Figure~\ref{ir_tx_schema} shows the physical arrangement of both links. The links face opposite one another and
-are shielded from one another by the motor's body in the center of the PCB.
-
-% We used an \texttt{MCP6494} quad CMOS op-amp. At a specified $\SI{2}{\milli\ampere}$ current
-% consumption it is within our rotor's power budget, and its Gain Bandwidth Product of $\SI{7.5}{\mega\hertz}$ yields a
-% useful transimpedance in the photodiode-facing TIA stage.
-
-\begin{figure}
- \begin{subfigure}{0.3\textwidth}
- \includegraphics[width=4.5cm]{ir_tx_schema.pdf}
- \caption{Basic layout, view along axis of rotation. 1
- - Rotor base PCB. 2 - Stator IR link PCB. 3 - Motor. 4 - receiver PIN photodiode. 5 - transmitter IR LED.}
- \label{ir_tx_schema}
- \end{subfigure}
- \hfill
- \begin{subfigure}{0.65\textwidth}
- \includegraphics[width=9cm]{photolink_schematic.pdf}
- \caption{Schematic with sample component values. C2 is highly dependent on the photodiode characteristics and
- stray capacitances.}
- \label{photolink_schematic}
- \end{subfigure}
- \caption{IR data link implementation}
-\end{figure}
-
-\subsection{Evaluation}
-
-The compoleted proof of concept hardware worked as intended. Both rotating power and data links worked well. As we
-expected, the mechanical design vibrated at higher speeds but despite these unintended vibrations we were able reach
-speeds in excess of $\SI{1000}{rpm}$ by clamping the device to the workbench. Even at high speeds, both the power link
-and the data links continued to function without issue.
-
-\section{Using MEMS accelerometers for braking detection}
-\label{sec_accel_meas}
-
-Using the proof of concept prototype from the previous section, we performed an evaluation of an \partnum{AIS1120}
-commercial automotive MEMS accelerometer as a braking sensor. The device is mounted inside our prototype at a radius of
-$\SI{55}{\milli\meter}$ from the axis of rotation to the center of the device's package. The \partnum{AIS1120} provides
-a measurement range of $\pm 120\,g$. At its 14-bit resolution, one LSB corresponds to $15\,\mathrm{m}g$.
-
-Our prototype IHSM uses a motor controller intended for use in RC quadcopters. In our experimental setup, we manually
-control this motor controller through an RC servo tester. In our experiments we externally measured the device's speed
-of rotation using a magnet fixed to the rotor and a reed switch held close. The reed switch output is digitized using an
-USB logic analyzer at a sampling rate of $\SI{100}{\mega\hertz}$. We calculcate rotation frequency as a
-$\SI{1}{\second}$ running average over debounced interval lengths of this captured signal\footnote{A regular frequency
-counter or commercial tachometer would have been easier, but neither was available in our limited COVID-19 home office
-lab.}.
-
-The accelerometer is controlled from the \partnum{STM32} microcontroller on the rotor of our IHSM prototype platform.
-Timed by an external quartz, the microcontroller samples accelerometer readings at $\SI{10}{\hertz}$. Readings are
-accumulated in a small memory buffer, which is continuously transmitted out through the prototype platform's infrared
-link. Data is packetized with a sequence number indicating the buffer's position in the data stream and a CRC-32
-checksum for error detection. On the host, a Python script stores all packets received with a valid checksum in an
-SQLite database.
-
-Data analysis is done separately from data capture. An analysis IPython Notebook reads captured packets and reassembles
-the continuous sample stream based on the packets' sequence numbers. The low $\SI{10}{\hertz}$ sampling rate and high
-$\SI{115}{\kilo Bd}$ transmission speed lead to a large degree of redundancy with gaps in the data stream being rare.
-This allowed us to avoid writing retransmission logic or data interpolation.
-
-Figure~\ref{fig-acc-steps} shows an entire run of the experiment. During this run, we started with the rotor at
-standstill, then manually increased its speed of rotation in steps. Areas shaded gray are intervals where we manually
-adjust the rotors speed. The unshaded areas in between are intervals when the rotor speed is steady.
-Figure~\ref{fig-acc-stacked} shows a magnified view of these periods of steady rotor speed. In both graphs, orange
-lines indicate centrifugal acceleration as calculated from rotor speed measurements. Visually, we can see that
-measurements and theory closely match. Our frequency measurements are accurate and the main source of error are the
-accelerometer's intrinsic errors as well as error in its placement due to construction tolerances.
-
-The accelerometer's primary intrinsic errors are offset error and scale error. Offset error is a fixed additive offset
-to all measurements. Scale error is an error proportional to a measurements value that results from a deviation between
-the device's specified and actual sensitivity. We correct for both errors by first extracting all stable intervals from
-the time series, then fitting a linear function to the measured data. Offset error is this linear function's intercept,
-and scale error is its slope. We then apply this correction to all captured data before plotting and later analysis.
-Despite its simplicity, this approach already leads to a good match of measurements and theory modulo a small part of
-the device's offset remaining. At high speeds of rotation this remaining offset does not have an appreciable impact, but
-due to the quadratic nature of centrifugal acceleration at low speeds it causes a large relative error of up to
-$\SI{10}{\percent}$ at $\SI{95}{rpm}$.
-
-After offset and scale correction, we applied a low-pass filter to our data. The graphs show both raw and filtered data.
-Raw data contains significant harmonic content. This content is due to vibrations in our prototype as well as gravity
-since we tested our proof of concept prototype lying down, with its shaft pointing sideways. FFT analysis shows that
-this harmonic content is a clean intermodulation product of the accelerometers sampling rate and the speed of rotation
-with no other visible artifacts.
-
-Figure~\ref{fig-acc-theory} shows a plot of our measurement results against frequency. Data points are shown in dark
-blue, and theoretical behavior is shown in orange. From our measurements we can conclude that an accelerometer is a good
-choice for an IHSM's braking sensor. A simple threshold set according to the sensor's calculated expected centrifugal
-force should be sufficient to reliably detect manipulation attempts without resulting in false positives. Periodic
-controlled changes in the IHSM's speed of rotation allow an offset and scale calibration of the accelerometer on the
-fly, without stopping the rotor.
-
-\begin{figure}
- \center
- \includegraphics[width=0.7\textwidth]{../../prototype/sensor-analysis/fig-acc-theory-meas-run50.pdf}
- \caption{Centrifugal acceleration versus angular frequency in theory and in our experiments. Experimental
- measurements are shown after correction for device-specific offset and scale error. Our measurements
- showed good agreement with our theoretical results. Above \SI{300}{rpm}, the relative acceleration error was consistently
- below $\SI{0.5}{\percent}$. Below $\SI{300}{rpm}$, the residual offset error that remains after our first-order
- corrections has a strong impact ($0.05\,g$ absolute or $8\%$ relative at $\SI{95}{rpm}$.)}
- \label{fig-acc-theory}
-\end{figure}
-
-\begin{figure}
- \begin{subfigure}{0.5\textwidth}
- \center
- \includegraphics[width=1.1\textwidth]{../../prototype/sensor-analysis/fig-acc-trace-steps-run50.pdf}
- \caption{Raw recording of accelerometer measurements during one experiment run. Shaded areas indicate time
- intervals when we manually adjusted speed.}
- \label{fig-acc-steps}
- \end{subfigure}
- \hfill
- \begin{subfigure}{0.45\textwidth}
- \center
- \includegraphics[width=1.1\textwidth]{../../prototype/sensor-analysis/fig-acc-trace-stacked-run50.pdf}
- \caption{Valid measurements cropped out from \ref{fig-acc-steps} for various frequencies. Intermodulation
- artifacts from the accelerometer's $\SI{10}{\hertz}$ sampling frequency and the $\SI{3}{\hertz}$ to
- $\SI{18}{\hertz}$ rotation frequency due to gravity and device vibration are clearly visible.}
- \label{fig-acc-stacked}
- \end{subfigure}
- \label{fig-acc-traces}
- \caption{Traces of acceleration measurements during one experiment run.}
-\end{figure}
-
-\section{Conclusion}
-\label{sec_conclusion}
-
-In this paper we introduced Inertial Hardware Security Modules (iHSMs), a novel concept for the construction of advanced
-hardware security modules from simple components. We analyzed the concept for its security properties and highlighted
-its ability to significantly strengthen otherwise weak tamper detection barriers. We validated our design by creating a
-proof of concept hardware prototype. In this prototype we have demonstrated practical solutions to the major electronics
-design challenges: Data and power transfer through a rotating joint, and mechanized mesh generation. We have used our
-prototype to perform several experiments to validate the rotary power and data links and the onboard accelerometer. Our
-measurements have shown that our proof-of-concept solar cell power link works well and that our simple IR data link
-already is sufficiently reliable for telemetry. Our experiments with an \partnum{AIS1120} automotive MEMS accelerometer
-showed that this part is well-suited for braking detection in the range of rotation speed relevant to the IHSM scenario.
-
-Overall, our findings validate the viability of IHSMs as an evolutionary step beyond traditional HSM technology. IHSMs
-offer a high level of security beyond what traditional techniques can offer even when built from simple components. They
-allow the construction of devices secure against a wide range of practical attacks in small quantities and without
-specialized tools. The rotating mesh allows longitudinal gaps, which enables new applications that are impossible with
-traditional HSMs. Such gaps can be used to integrate a fan for air cooling into the HSM, allowing the use of powerful
-computing hardware inside the HSM. We hope that this simple construction will stimulate academic research into (more)
-secure hardware.
-
-\printbibliography[heading=bibintoc]
-
-
-%%% FIXME remove appendix and work into text.
-
-\center{
- \center{This is version \texttt{\input{version.tex}\unskip} of this paper, generated on \today. The git repository
- can be found at:}
-
- \center{\url{https://git.jaseg.de/rotohsm.git}}
-}
-\end{document}
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-\documentclass[10pt,journal,a4paper]{IEEEtran}
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-
-\begin{document}
-
-\title{Tech Report: Inerial HSMs Thwart Advanced Physical Attacks}
-\author{\IEEEauthorblockN{
- Jan Sebastian Götte\IEEEauthorrefmark{1}\IEEEauthorrefmark{2} \and
- Björn Scheuermann\IEEEauthorrefmark{1}\IEEEauthorrefmark{2}
- }\\
- \IEEEauthorblockA{
- \IEEEauthorrefmark{1}Alexander von Humboldt Institut für Internet und Gesellschaft (HIIG)\\
- \IEEEauthorrefmark{2}Humboldt-Universität zu Berlin\\
- \texttt{\textbf{\small goette@jaseg.de}}, \texttt{\textbf{\small scheuermann@informatik.hu-berlin.de}}
- }
-}
-\date{2021-01-05}
-\maketitle
-
-\section*{Abstract}
-
-In this tech report, we introduce a novel countermeasure against physical attacks: Inertial hardware security modules
-(iHSMs). Conventional systems have in common that they try to detect attacks by crafting sensors responding to
-increasingly minute manipulations of the monitored security boundary or volume. Our approach is novel in that we reduce
-the sensitivity requirement of security meshes and other sensors and increase the complexity of any manipulations by
-rotating the security mesh or sensor at high speed---thereby presenting a moving target to an attacker. Attempts to stop
-the rotation are easily monitored with commercial MEMS accelerometers and gyroscopes. Our approach leads to a HSM that
-can easily be built from off-the-shelf parts by any university electronics lab, yet offers a level of security that is
-comparable to commercial HSMs.
-
-This tech report is the abridged version of our forthcoming paper.
-
-\section{Introduction}
-
-While information security technology has matured a great deal in the last half century, physical security has barely
-changed. Given the right skills, physical access to a computer still often means full compromise. The physical
-security of modern server hardware hinges on what lock you put on the room it is in.
-
-Currently, servers and other computers are rarely physically secured as a whole. Servers sometimes have a simple lid
-switch and are put in locked ``cages'' inside guarded facilities. This usually provides a good compromise between
-physical security and ease of maintenance. To handle highly sensitive data in applications such as banking or public key
-infrastructure, general-purpose and low-security servers are augmented with dedicated, physically secure cryptographic
-co-processors such as trusted platform modules (TPMs) or hardware security modules (HSMs). Using a limited amount of
-trust in components such as the CPU, the larger system's security can then be reduced to that of its physically secured
-TPM~\cite{newman2020,frazelle2019,johnson2018}.
-
-Like smartcards, TPMs rely on a modern IC being hard to tamper with. Shrinking things to the nanoscopic level to secure
-them against tampering is a good engineering solution for some years to come. However, in essence this is a type of
-security by obscurity: Obscurity here referring to the rarity of the equipment necessary to attack modern
-ICs~\cite{albartus2020,anderson2020}.
-
-HSMs rely on a fragile foil with much larger-scale conductive traces being hard to remove intact. While we are certain
-that there still are many insights to be gained in both technologies, we wish to introduce a novel approach to sidestep
-the manufacturing issues of both and provide radically better security against physical attacks. Our core observation
-is that any cheap but coarse HSM technology can be made much more difficult to attack by moving it very quickly.
-
-For example, consider an HSM as it is used in online credit card payment processing. Its physical security level is set
-by the structure size of its security mesh. An attack on its mesh might involve fine drill bits, needles, wires, glue,
-solder and lasers~\cite{drimer2008}. Now consider the same HSM mounted on a large flywheel. In addition to its usual
-defenses the HSM is now equipped with an accelerometer that it uses to verify that it is spinning at high speed. How
-would an attacker approach this HSM? They would have to either slow down the rotation---which triggers the
-accelerometer---or they would have to attack the HSM in motion. The HSM literally becomes a moving target. At slow
-speeds, rotating the entire attack workbench might be possible but rotating frames of reference quickly become
-inhospitable to human life. Since non-contact electromagnetic or optical attacks are more limited in the first place and
-can be shielded, we have effectively forced the attacker to use an attack robot.
-
-In Section~\ref{sec_related_work}, we will give an overview of the state of the art in the physical security of HSMs. On
-this basis, in Section~\ref{sec_ihsm_construction} we will elaborate the principles of our inertial HSM approach. We
-conclude this paper with a general evaluation of our concept in Section~\ref{sec_conclusion}.
-
-\section{Related work}
-\label{sec_related_work}
-% summaries of research papers on HSMs. I have not found any actual prior art on anything involving mechanical motion
-% beyond ultrasound.
-
-In this section, we will briefly explore the history of HSMs and the state of academic research on active tamper
-detection.
-
-HSMs are an old technology tracing back decades in their electronic realization. Today's common approach of monitoring
-meandering electrical traces on a fragile foil that is wrapped around the HSM essentially transforms the security
-problem into the challenge to manufacture very fine electrical traces on a flexible foil~\cite{isaacs2013, immler2019,
-anderson2020}. There has been some research on monitoring the HSM's inside using e.g.\ electromagnetic
-radiation~\cite{tobisch2020, kreft2012} or ultrasound~\cite{vrijaldenhoven2004} but none of this research
-has found widespread adoption yet.
-
-In~\cite{anderson2020}, Anderson gives a comprehensive overview on physical security. An example they cite is the IBM
-4758 HSM whose details are laid out in depth in~\cite{smith1998}. This HSM is an example of an industry-standard
-construction. Although its turn of the century design is now a bit dated, the construction techniques of the physical
-security mechanisms have not evolved much in the last two decades. Besides auxiliary temperature and radiation sensors
-to guard against attacks on the built-in SRAM memory, the module's main security barrier uses the traditional
-construction of a flexible mesh wrapped around the module's core. In~\cite{smith1998}, the authors state the module
-monitors this mesh for short circuits, open circuits and conductivity. The fundamental approach to tamper detection and
-construction is similar to other commercial offerings~\cite{obermaier2018,drimer2008,anderson2020,isaacs2013}.
-
-To the best of our knowledge, we are the the first to propose a mechanically moving HSM security barrier as part of a
-hardware security module. Most academic research concentrates on the issue of creating new, more sensitive security
-barriers for HSMs~\cite{immler2019} while commercial vendors concentrate on means to certify and cheaply manufacture
-these security barriers~\cite{drimer2008}. Our concept instead focuses on the issue of taking any existing, cheap
-low-performance security barrier and transforming it into a marginally more expensive but high-performance one. The
-closest to a mechanical HSM that we were able to find during our research is an 1988 patent~\cite{rahman1988} that
-describes a mechanism to detect tampering along a communication cable by enclosing the cable inside a conduit filled
-with pressurized gas.
-
-\section{Inertial HSM construction and operation}
-\label{sec_ihsm_construction}
-
-Mechanical motion has been proposed as a means of making things harder to see with the human eye~\cite{haines2006} and is
-routinely used in military applications to make things harder to hit~\cite{terdiman2013} but we seem to be the first to
-use it in tamper detection. If we consider different ways of moving an HSM to make it harder to tamper with, we find
-that making it spin has several advantages.
-
-First, the HSM has to move fairly fast. If any point of the HSM's tamper sensing mesh moves slow enough for a human to
-follow, it becomes a weak spot. E.g.\ in a linear pendulum motion, the pendulum becomes stationary at its apex. Second,
-a spinning HSM is compact compared to alternatives like an HSM on wheels. Finally, rotation leads to easily predictable
-accelerometer measurements. A beneficial side-effect of spinning the HSM is that if the axis of rotation is within the
-HSM itself, an attacker trying to follow the motion would have to rotate around the same axis. Their tangential linear
-velocity would rise linearly with the radius from the axis of rotation, which allows us to limit the approximate maximum
-size and mass of an attacker using an assumption on tolerable centrifugal force. In this consideration the axis of
-rotation is a weak spot, but that can be mitigated using multiple nested layers of protection.
-
-\begin{figure}
- \center
- \includegraphics{concept_vis_one_axis.pdf}
- \caption{Concept of a simple spinning inertial HSM. 1 - Shaft. 2 - Security mesh. 3 - Payload. 4 -
- Accelerometer. 5 - Shaft penetrating security mesh.}
- \label{fig_schema_one_axis}
-\end{figure}
-
-In a rotating reference frame, centrifugal force is proportional to the square of angular velocity and proportional to
-distance from the axis of rotation. We can exploit this fact to create a sensor that detects any disturbance of the
-rotation by placing a linear accelerometer at some distance from the axis of rotation. During constant rotation, after
-subtracting gravity both acceleration tangential to the rotation and along the axis of rotation will be zero.
-Centrifugal acceleration will be constant.
-
-Large centrifugal acceleration at high speeds poses the engineering challenge of preventing the whole thing from flying
-apart, but it also creates an obstacle to any attacker trying to manipulate the sensor. We do not need to move the
-entire contents of the HSM. It suffices if we move the tamper detection barrier around a stationary payload. This
-reduces the moment of inertia of the moving part and it means we can use cables for payload power and data. Even at
-moderate speeds above $\SI{500}{rpm}$, an attack would have to be carried out using a robot.
-
-\subsection{Mechanical layout}
-
-Thinking about the concrete construction of our mechanical HSM, the first challenge is mounting both mesh and payload on
-a single shaft. The simplest way we found to mount a stationary payload inside of a spinning security mesh is a hollow
-shaft. The payload can be mounted on a fixed rod threaded through this hollow shaft along with wires for power and
-data. The shaft is a weak spot of the system, but this weak spot can be alleviated through either careful construction
-or a second layer of rotating meshes with a different axis of rotation. Configurations that do not use a hollow-shaft
-motor are possible, but may require additional bearings to keep the stator from vibrating.
-
-The next design choice we have to make is the physical structure of the security mesh. The spinning mesh must be
-designed to cover the entire surface of the payload, but compared to a traditional HSM it suffices if it sweeps over
-every part of the payload once per rotation. This means we can design longitudinal gaps into the mesh that allow outside
-air to flow through to the payload. In traditional boundary-sensing HSMs, cooling of the payload processor is a serious
-issue since any air duct or heat pipe would have to penetrate the HSM's security boundary. This problem can only be
-solved with complex and costly siphon-style constructions, so in commercial systems heat conduction is used
-exclusively~\cite{isaacs2013}. This limits the maximum power dissipation of the payload and thus its processing power.
-Our setup allows direct air cooling of regular heatsinks. This greatly increases the maximum possible power dissipation
-of the payload and unlocks much more powerful processing capabilities. In an evolution of our design, the spinning mesh
-could even be designed to \emph{be} a cooling fan.
-
-\subsection{Spinning mesh power and data transmission}
-
-On the electrical side, the idea of a security mesh spinning at more than $\SI{500}{rpm}$ leaves us with a few
-implementation challenges. Since the spinning mesh must be monitored for breaks or short circuits continuously, we need
-both a power supply for the spinning monitoring circuit and a data link to the stator.
-
-We think that a bright lamp shining at a rotating solar panel is a good starting point. In contrast to e.g.\ slip
-rings, this setup is mechanically durable at high speeds and it also provides reasonable output power. A battery may not
-provide a useful lifetime without power-optimization. Likewise, an energy harvesting setup may not provide enough
-current to supply peak demand.
-
-Since the monitoring circuit uses little current, power transfer efficiency is not important. On the other hand, cost
-may be a concern in a production device. Here it may prove worthwhile to replace the solar cell setup with an extra
-winding on the rotor of the BLDC motor driving the spinning mesh. This motor is likely to be a custom part, so adding
-an extra winding is unlikely to increase cost significantly. More traditional inductive power transfer may also be an
-option if it can be integrated into the mechanical design.
-
-\begin{figure}
- \center
- \includegraphics{ir_tx_schema.pdf}
- \caption{Example of a bidirectional IR communication link between rotor and stator, view along axis of rotation. 1
- - Rotor base plate. 2 - Stator base plate. 3 - Motor. 4 - receiver PIN photodiode. 5 - transmitter IR LED.}
- \label{ir_tx_schema}
-\end{figure}
-
-Besides power, the data link between spinning mesh and payload is critical to the HSM's design. This link is used to
-transmit the occassional status report along with a low-latency alarm trigger (``heartbeat'') signal from mesh to payload.
-A simple infrared optical link as shown in Figure~\ref{ir_tx_schema} may be a good solution for this purpose.
-
-\section{Conclusion}
-
-\label{sec_conclusion} To conclude, in this tech report we introduced inertial hardware security modules (iHSMs), a
-novel concept for the construction of highly secure hardware security modules from inexpensive, commonly available
-parts. We elaborated the engineering considerations underlying a practical implementation of this concept.
-
-Inertial HSMs offer a high level of security beyond what traditional techniques can offer. They allow the construction
-of devices secure against a wide range of practical attacks at prototype quantities and without specialized tools. We
-hope that this simple construction will stimulate academic research into secure hardware.
-
-\printbibliography[heading=bibintoc]
-\appendix
-
-\subsection{Patents and licensing}
-During development, we performed several hours of research on prior art for the inertial HSM concept. Yet, we could not
-find any mentions of similar concepts either in academic literature or in patents. Thus, we are likely the inventors of
-this idea and we are fairly sure it is not covered by any patents or other restrictions at this point in time.
-
-Since the concept is primarily attractive for small-scale production and since cheaper mass-production alternatives are
-already commercially available, we have decided against applying for a patent and we wish to make it available to the
-general public without any restrictions on its use. This paper itself is licensed CC-BY-SA (see below). As for the
-inertial HSM concept, we invite you to use it as you wish and to base your own work on our publications without any fees
-or commercial restrictions. Where possible, we ask you to cite this paper and attribute the inertial HSM concept to its
-authors.
-
-\center{
- \center{\ccbysa}
-
- \center{This work is licensed under a Creative-Commons ``Attribution-ShareAlike 4.0 International'' license. The
- full text of the license can be found at:}
-
- \center{\url{https://creativecommons.org/licenses/by-sa/4.0/}}
-
- \center{For alternative licensing options, source files, questions or comments please contact the authors.}
-
- \center{This is version \texttt{\input{version.tex}\unskip} generated on \today. Once the full paper has been
- published, this project's git repository will be available at:}
-
- \center{\url{https://git.jaseg.de/rotohsm.git}}
-}
-\end{document}
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