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REPRODUCED FROM BEST AVAILABLE COPY
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USTE[ALS AND CO!VOXWHSs PAW I
E:" IAUTHOR81 CLIDS 0, SNAW
~SOLID STATE ZLMTRONIC DEPTO
ID
ISSIEXLE SYSTEMNS DIVISIO
I S U N N Y V ALE C A LAI P0 R N IA
ii
JE16# 2958-
31CWI R&DUIOtIQ LSFMOTON INFPRUREYATEFtIAis AND CIWIO~iAT5# PAIR I
ZF1'DT OF GAMOA, RADUI&TON ON IMPRAREDTR&NSX=TTNG 1409RIALS AND FILTERS
AUTB'RM CLnhS 0 * SRARl a. MWTUO~DSOLID STATIC RLETONCZ W319
£LRTRONXCS DIVSIONRMEARC AKUDEMPME1W BRANCH
LOux E )K8S=L 873TE2 DIVISIONPAID ALTO, CALICQMXA
Fag*
INT1ODUCTIOREXPIMfl4?A PHOUO R2~R 2R S 3
OONOLUSIOI48 7
Figur* 1 Optical Transmiasion Spectrwa of Corning
In?905 Vycor8
Figure 2 Optial Traamaission Spectrum of warts -
Figure 3 Optioal Transmission Spectrum of Crming ?uedSilica 9
Figure 4 Optical Transmission Spectrum of 0alaivmAluminate Glass 10
Figure Optical Transmisuion Spectra of Arnic 1
Figurt 6 Optical Transmission Spectrum of SeleniumGlass 11
Figure 7 Optical Transmission Spectrum of Magnesia0dde 11
Figur Optial Transmission Spectrum of Sapphire 12
Figure 9 Optical Transmission Spectrum of Silicon 12
Fngure 10 Optical Transmission Spectrum of Dauscki &Lomb Filter 3a 13
Figwe 21 Optical Transmission Spectrui of Bausoh & LambFilter 8173 13
Figure 12 Optical Transmission Spectrum of Bausch & LombFilter 4 14
Figure 13 Optical Transmission Spectrum of Bausch & LombFilter 113M 114
A Figure, 14 Optical Transmission Spectrum of Bausch &LombFilter 8014
Figurv 15 Optical Tranhmission Spectrum of Bausch & LombFilter 8233
ngws 16 Optical Transais ion Spectrum of Bavoh & Lo*1Filter 96 6
?igur 17 Optical TrMiuoesioi Spectrum of Baich & Lob1Filter 794 6
FngwM 18 Optioal Transiss.on Spectrum of BaUreh & LOb_Plter 7899 17
l 9 opical Transmission Spectrum of O*ori% Fiter2.61 17
Ftgwo 20 Optical TTrsax ieon Spectrm of Gaoing Filter li
Fire 21 Optical Tran ssion Spectrum o orni filter 18
rigure 22 optical Trn smission Spectrum of CoT14i Filter 19
ftgue 23 Optdioa2 fransmaisil Spectra of Ponu Fiter
r. 19
Fgwe 24 Optical Trasmssion Spectrum of Jows l1opIa
Filter 20
Ma - OpU4 iclramiesioU $O 0n~w M pwtCeviwHor. 20
LMSO No: WA No: Government Security50114 8723 Classification of Report
Date: No of Pages: Unclassified6-16"51 20
Titleo: Nuclear Radiation Effects on Infrared Materials ondomrponentep Part I& Effects of Gamma Radiation on Infraredrransmittixag Materials and Filters*Author(s): Clyde C. Shaw and R.". RAOgDepartment: Solid State Sleotronice No.Division: Electronics
Author's Do artment Appoval for:Approval Nu Release Only 0 a E an- s
Department Manager -!n - - -- - -- --
Summnary of Report
Results of a survey of cobalt-60 gamn- radiation_effects on the optical properties of it number of
i1nfrared- transmitting -materials -and--f ilters -are-presented*
This study shows that, with few exceptions$ thematerials and filters are intsensi ive to gammiaradiation at a dos age lovel of, 101 roentgens ormore*
SECURITY CLASSIFICATION OF SUMEARY None
LMSD-
DISTRIBUTION FOR U4CLASSIFIED REPORTS'I_ SOLID STATE ELIZTRONICS DEPARTMENTABSTRACT
PAE FULLONLY PORT STANDARD DISTPTBUTION DT-
1 Chief Scientist, L. N. Ridenour 10-011 - Deputy Chief Scientist, D. T. Perkins 10-011 - Chief Scientist - Staff, K. T. Larkin 10-10- 1 Director, Research and Development Branch, R. Smelt 50-012 - Senior Scientific Advisor, CORIAC, Larmour, Lewis 01-14
Associate Director Spacecraft and Missile Research,- 1 W. C. Griffith 53-01
Associate Director, Communications and Controls Research1 J. P. Nash 54-01
Associate Director, Advanced Systems Research,- 1 S.H. Brown 55-01
1 Manager, Technical Staff, T. Teichmann 50-20Manager, Flight Sciences Division, W. C. Griffith
I - (Acting) 53-10! - Manager, Physics Division, F. C. Hoyt 53-20- 3I Manager, Electronics Research Division, W. F. Main 54-10- Manager, Electronics Application Division,
I De B. HoffmanManager, Mathematics and Information Processing,
1 J. P. Nash (acting) 54-306 1 Manager, Radar and Data Link Department, R. L. Vader 54-118 1 Manager, Electromagnetics Department, E. A. Blasi 54-12
Manager, Solid State Electronics Department,2 1 C. F. Spitzer 54-13
---- 1 - Manager, Computer Development Department, A, 8. Zukin 54-15-Manager, Instrumentation Application Department,
I - De B. Hoffman (acting) 54-201i - Manager, Telecommications Department, J. W. Muehlner 54-22S- Manager, Guidance Department, R. L. Vader (acting) 54-23
20 1 Head, Solid State Devices Section,C. F. Spitzer (acting) 54-13
20 1 Head, Solid State Physics Section, H. N. Leifer 541315 ! Head, Infrared Section, L. H. Chasson 54-1310 1 Head, Electrochemistry Section, M. Eisenberg 54-13-- 6 R&D Technical Information Center 50-91-- I H. E. Shaw, Technical Publications Dept. 50-91-- .I Library: GELAC-- 1 Library: CALAC
Technical Director, Development Division, XA,1 F. W. O'Green 62-10
Technical Director, Development Division, XN,1 F. J. Bednarz 66-10
Technical Director, Development Divisions XP,1 T. J. Anderson 63-30
NUCLIAR RADIATION ZFlUOS ON IVFAR
NATMUALS AND COMPONUTSs AD? I
UFWTOF 0? WA RADITIO c*I Inow=
TSAMWNTZ )%ATMIAL AND MXERIS
The Infrared system designer is confronted vith a number of problm
arising froa interactions of the system with the miramt In which bit
device is required to operate. An iscreasingly Imnportmnt addition to the
Catalog of eniromaital effects is that du. to nuclear radiation. Tho
importance of considering the effects of thias vxcim becomes appareit
whevr the ayma t bdesindto oporate inthe vicizilrof a
source of nuclear radiationk mach an a nuclear power source.
-It-mas iAth- the puzrpose in uind--of-pvdingtthe into-riatcia zul--
to the infrared sat m cesgmer that a &tudy of nucleam radiation ffeaoW
an infrared materia.1s end ceponents was initiated at the Lockheed Missile
S ystem Divieion Research Laboratories*
It is proposed that the recults of this investigation be presented in
a series of reportsp of which this is tb- first. These reports viiU
include gaa=a-ray and neutron radiation damngo to Infrared transmitting
*
naterials, filters and detectors. As new and interesting materials and
components become available the ill be evaluated and the results
included in periodic supplementary reports.
This first report vi l be confined to a study of the effects of
gama- raiation-an the -infrared tranaiai -of optical materials_ ad
infrared fiters. It in presented as a mwvey of a number of useful
infrared materials, rather than as a scientific study or a tutorial
article. For inforution of this character, the reader is referred to a
recent publication by G. J. Diener and G. H. Vineyard, Radiation Effects
i lds4a 1 Interscienee Publbshers, Ino., New York, 1957, and the -.acluded
bibliographq.
Infrared tranu±51onk curres of the optical materials and filters
wen obtained before and after axposure to radiation. In this study a
double-passs csnle-boax Perkin-lmar Model #132 Universal Infrared
Spectromter was used. This instrument employed a globar source# a rock-
salt prisl, and a thermocouple detector with a O~r vindow. The xpe ri-
metal error in determining transmittance as a function of wavelength taes
found to be less than 4%.
The samples were irradiated by exposure to cobalt-60 gamma radiation
in the Lockheed Niasile Systems Division 100 curie facility. Dosmetry
measuremants on this source show that a maximum dose rate of 2 X
roentgens/hr can be obtained for small samles. However, in this study a
2
AN
dose rate of MO5 rootgenu/br va used. Irradiations and spectral trans-
mission meamemets we, all conducted at room temperature.
In addition to the gamma irradiation studies, an available polonium-
beryllua source was used in a low-flux neutron irradiation investigation
of the optical materials. A neutron flux of 0/ca2 se. va obtained
from this soiwce.
Selection of infrared optical materials to be tested n this study
was based cn a mimbeor of factors. Consideration was given to all materials
vith optically useful tranm2AXtances in some region of the infrared
spectrum above 2 microl J however, the ver7 hygroscopic and the Yore
chemically, or ther=lly, unstable sub tances were ruled out.
The aocoManying traramission curves show the percent transmission as
a function of vavelagth for the materials tested. The infrared trans-
- mittanoes- of -ri:,st of -the--substanoes -examined- vere, --for aU-practical
purposes, unaffecte by A total accumlated gamnu dosage of 2 1 107
roentgens. In the interest of caleteness, the cues of all aterials
examined, including those not affected by radiatlon, are shon.
The folloVing infrared materials were studiedt
1) . 1 This product of COning Glass W rks avoids the strong
absorption band at 2.7 microns that is a characteristic of most silica
glasses. A gama dose of 2 I 107 roentgens rendered it opaque in the
visible region of the Mpcotrum, but produced only a very slight
3
depression in its infrared tranvilttanoe. The radiation induced
transmission properties of this mterial# shown to be relative17 stable
below about 2500 0, ma have posible applications an band-pass filters
in the near infrared region.
2) & ost A nmber of amples of oosmroially avAilable quarts (Am*rill
General Elsotrio, ae.) We" e ayedo The post-rradiation& trans..
mission curves shoved the an opacity In the visible region as did the
,) o .lo This atriaW, recently developed by OorTnag Glass Worbk
and claisad to be 100 pus Si02., was apoaod to a tal gams dosage
of 108 roontgns with no observable effects in its infrared transmission
r piopertiss. It hW been suggested that this unique resistance to
radiation damage results from the abseno of impurities normally found
In quats and glass.
- 14 ~Oloim Auu~nte 2*0* Anumber -of -types- of-calcium -eliminate
(M-100lo 110 120 2# 20), supplied by Dausch & Lomb Optical CoMpmy were
studioed, All samples were, within the eperiental error, found to be
unaffected by gum dosages of 07 ro1tgaszis A typical tras.mision
curve is shem.
5)Arsenic Trivt,!Mse03assv Samples of this mterials available frost the
Servo Oorportion of Asteroa under the trade nme "Bew-rofra0x0t sOVd
no ohawie in optical propertios after & 2 X 10 *oetg.n gamm dos.
14
6) Selenium Maye Eastan Kodak Company has reoh!ly dveloped an areoan-
selenium glass with an index of refraction of 2*.4 or higher, md a
transmittance that is optically us ful out to 25 microns.
The aocwceraing curve shows its transmittanoe, which showed no
ohange after 107 roentgens, out to the long-wavelt imit of t0apootrmt r.
7) !w su.oio Samples of )Igo (Periclas) were obtained fr*A Weo
soUrCes. Ligh-purity optical quality arystals splied by the Infraed
Developmnt Owpoa, England# appeared completey resistant to gam
radiation at a dosage level of 2 X 107 roeantge, Hovevor# this dosage
indwed an absorption band rear 2*0 microns in commoer" rad
magnesium aide obtained from Nort-n Coaeny.
8) L, Thin windows of A,203 #uPU d Linde Air Protd .p sd"O,
were eoposed to a gum dosage of 2 X 107 roentgens with no' omarbial
Vwnows of Texa Irstrum InTorporated ftliton remained unoh ed
after 2 X 107 roentgens.
A representative number of various typee of infrared filters were
evaluated with respect to gam radiatio offet**
a5
The spectral tranoeattmnoe of each filter was obtained before and
after oposure to an aocu i ated gamma dosage of 107 roentgens. ithin
lAits of expe r umtl error, the infrared tranwasiom properties of afl
smples tested remained unchanged, both with respect to radatio-induced
infrard absorption bands and detuning effects. Again, infrared trana-
-ssi- ncu orre have be included which plot percent tranwiuamt m as a
notiom of aveolength in airone,
Two types of filters wre =amined. These included Bausch & Lomb
1nterfrane filters, and glass absorptio filter from Corning OIas, The
first type w be obtained either as bandpaso filters or as longavele-gth.
pass filters, Proe oambinzatis of the two types result in composite
c filters with clean, single-band tr muissio h baraterieticis.
Also ahow In thie report axe the tranw asicn crvee of two Itiple-
lv.w l teferfee filters devtloped br R. G. OreeiePlJ)of Johns Hopin
Uhiveeit7, .
With reference to tbe results of the previously metioned lov-flux
noutc Lrradatin stwy, it carn as o svxprise that integrated fluxes of
2 X UPZ0 ca produoed no observable effeots. This phase of the investiga-
tion will be exw ded to include high-flux neutron iradlations*
(1) Om.er* , R. 0., ,. Opt. Sot. qo, 788(l95)s as 130(2957)
6
The ravults of this study show that, with few .excep*4cwi infrared
I optical waterial.s and filters are insenuitive to game radiation at a donage
level of 2. oentgenis or 'ioe. In thoue cases i*are the optical properties
-we gfete4 tw -changes awe not racessarily 4wtrautl. to the operation
of infrared estem. aloying these particular saterials#~ .
A nOtq of cautioni Ath regard to the bavior of saof he
zatw~'*' JA particular substances containing vilica, appears to be I
S order* A study oonduet*4 at the Boeing Airpane Ca~any has U~icated tha
wexto of luminous ewiation from a u~mber of optioal mtoriLU =mr
gemsu banbardwint, It is proposed that this effet vdill be investigate as
Spart of the geiwre2. nulear radi~ation stuidy at a future data#
(2) Barton, J, A. and Steele, H.L., Boeing Rapt D2,.662 (Jan. 11p 1957)
1 7
U-)U,
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ODHNOISMRNVJl
00
360
4 0 /-40/
20CRIN FUSEDSILICTHICKNESSE~ 6.mm
WAVLENTH( MICRONS)
CALCIUM ALUMINATE GLASSTHICKNESS ROmmi
WAVELENGTH (MICAMNS)
go -
j40-ANSENIC TYRIOULPID
go-TH4ICKNESS Z.5mn
2 4 6 8 10 12 t4 14 le 20WAVELENOTH (MICRONS)
Fir,5 (I~lca Tra~aimrusj :jiantium o /minia 'ri Ul-
100
0
a 40- SELENIUM GLASSTHICK~NESS 3.5 mm
WAVELE~NGTH (MICRONS)Fi.6 Optioal Tiatmatb tporit~m of' 8#2.rnlm Obihm
10
60 /
40
MAGNE~SIUM OXIDETHICKNESS Imm
20 - - BePORL
0ATE 20
WAVELENGTrH (MICRONS)na. I Optia±l Trmpkisai ipetra3 at Mspcilum Osido
20- APPHIRU20 THICKNESS 2mm.
WAVELENGTH (MICRONS)B Op icl Tr, iiniidnaiin !lroti-mo of3pih
100,
so
40-
20 - THICKNESS Omm,
0 2 4 6 8 1 12 14 16 to 2
WAVELENGTH (MICRO0NS)
rig 9 tidal 'Trwimiiiiofl anam ofw st i]lon
80-
80 -
BAUSCH a LOM13 FILTER Uz
WAVMLNOTH (MICROWNI1% WC Optical TVp fLvpMntl . rpoctm Of' llaunch Lm FiVltoiw I
60-
40
BAUSCH 8 LOMB FILTER 817 320
10.0304.0 8.0 0
01.0 2,0 WAVELENOjTH (I CRONS)10.nit 11 opt1ii. TJnflmllaoli Specinm~ of 1unch & 6,mh h'1tor 8173
so-
40
~40 BAUSCH A LOMB FILTER 4
20
WVELENGTH (MICRON$)i~U 12 OpUipk Trmmieo .~ patrupi of Bnxuaah 4 Lamb Filter 14
20- IBAUSCH 5 LOMS FILTER 113N
2.0 3.0 4.0 &~ 0OWAVE.LENGTH (MICRONS)
Mg 13 Opin Trivimliin 5potrump of flisah &. Ipmb Filter 1tI3
80
340-20-
BAUSCH a LOOA FILTER 804
110 2,0 304.0 5.0 600WAVELENGTH (MICRONS)
Fi-1 Optigal TmviIion Spotrm or Vausoh & tomb 'Flter ON
10
2 Go-
40-
BAUSCH aLOMB FILTEP 0l233
20
01.0 210 & . . .
WAVtLENGTH (MICRONS)ig1 Optical Trlwnaion Spectum of fausch 6 Lotab Filtar 0233
0-60
z4
40-
20 -BAIUSCH SLOMB FILTER 96
010 203-0 4.0 50 s
WAVELENGTH (MICRONS)P-le. 16 Optical ?ran-saission Spectrum of lPausch &Lm Filter 96
0
z0 -0
1 40-
BAUSCH 8 LOMB FILTER T944
20-
0 -210 3.0 40 so 6.0WAVSLENGTI4 (MICRONS)
Fng. 17 Optical Transmission Spectrum of Dauisch & Lnmb Filter 7944
16
100
so
BAUSCH4 & LOMD FILTER 7599
40
20
1.0 acS0 4.0 510 6.0
WAVELENGTH CMICI4ONS)* Fig. 15 Otloal 'Tra1m~bor 3pfqint ru of llaundh kwi ?(M~tor 7899
so OCANINO FILTER 9-01
40I 4
20
0 -/0 1 2 34 5
WAVELENGYN (MICRONS)Ttg# 39 DI~la~d jTraoii seoatr~m or Coin Piltor 2..61
100
so CORNING FILTER 7-57
60
20
0 1 2 3 4 5-' WAVELENGTH (ICRONS)
Fig. 20 Optical Trajraftooian Spectrum of Coning Pilter 7-57
COMMN$ FILTER 7-57
40
20
0 I2 3 4 5WAVELENGTH (MICiquoNS)
Fig$ 21 Opticil Tronsmis-ioi npoetrm of Corning Filter 7-57is
100
60-
960-
140
oL0 I34
WAVELENGTH (MICRNS)Fig. 22 aptiosi. T rnIthidh 8pntim of coiIlp l1Iwnl' ) l
1419
I00
so
toJOHN$ HOPKINS FILTER
20
0 a 4 6 10 12 14 Is Is to
WAVELENGTH (MICRONS)
so
,JOHNS H0!%KIN3 FIIRTt
do$40
20
2 4 6 a 10 la 14 to Is 20
WAVELENOTH (MICRONS)Pi.2 Optial T raom amton~ ptr tm o Jor m lnh iwki m I to~l~r