Gei g er T ube T heo r y , Dead T i me
22. S 902 – D I Y G eiger C ount ers P rof . M ic hael S hort
Quest i o ns t o St ar t
Wher e i s t he be st pl ac e t o ex t r a c t our c ount r a t e si gnal ?
What i s t he hi ghe st c ount r a t e t ha t w e
c an det e c t ?
Courtesy of Mark Chilenski. Used with permission. 2
M o t i vat i o n
U nders t and how ioniz at ion c ham bers , and s pec if ic ally G eiger t ubes , f unc t ion
Learn t he m ec hanis m of “dead t im e” in det ec t ors , and how it lim it s t hem
C harac t eriz e det ec t ors as paraly z able or not
P redic t how dead t im e w ill af f ec t c ount ing out put and s t at is t ic s
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Gei g er- M üller T ubes
http://www.imagesco.com/geiger/gmt -0 3.jpg
A n SB M -2 0 U tu b e , s h o w i n g th e w i re a n o d e
Courtesy of Im age s SI, Inc. Used wit h p ermission.
O u r SBM- 20
Geiger t ubes 4
O ur SBM - 20 Gei g er- M üller T ubes
W a l l t h ickn e ss: 50 µ m st e e l W a l l De n sit y: 8 g/c m 3 Assu m e 1 at m equa l ga s mi x ture
T u b e d i ag ram © so u rce u n k n o w n . A l l ri g h ts re se rv e d . T h i s con te n t i s excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/help/faq -f air -u se/ .
For m or e inf or m a t ion, s e e : h ttp : //www .gs t ube .c om /da t a /2 3 9 8 /
Io ni zat i o n Chamber s
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Geiger tube photo courtesy of Jeff Keyzer on F lickr. – +
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Circuit diagram © Wiley-VCH, from J. Turner, Atoms, Radiation, and Radiation Protection (2007). All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/help/faq-fair-use/ .
T he Io ni zat i o n P lat eau ( L o w- V )
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T he Io ni zat i o n P lat eau ( M ed - V )
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T he Io ni zat i o n P lat eau ( H i g h- V )
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T he Io ni zat i o n P lat eau ( H IGH - V )
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No w fo r t he M at h…
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𝑐 𝑚 2 − 𝑠
Let' s s ay a gamma fl ux of Φ ̇ enters a c hamber of area A .
E ac h mak es N i on pai r s , eac h w i th a c har ge of e and ener gy W ,
an d th en s tops i n the c ham be r:
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W ̇ = Φ ̇ 𝐸 γ
R a d i a ti o n “ I n te n s i ty ”
The c har ge produc e d per parti c l e i s 𝑁𝑒 , and t he number of
parti c l es enteri ng per s ec ond i s Φ ̇ 𝐴 . That mak es the c urrent I :
𝐼 = Φ ̇ 𝐴 𝑁𝑒
Let' s s ay a
gamma fl ux of Φ ̇
enters a c hamber of area A .
E ac h mak e s N i on pai r s , eac h w i th a c har ge of e and ener gy W ,
and then s t ops i n the c ham ber:
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W ̇ = Φ ̇ 𝐸 γ
“ I n te n s i ty ”
R a d i a ti o n
N ow us e t he radi ati o n in t e n sit y:
No w fo r t he M at h…
#
𝑐 𝑚 2 − 𝑠
𝐼 = Φ ̇ 𝐴 𝑁𝑒
𝐼
𝐴 𝑁𝑒
= Φ ̇
W ̇ = 𝐼
𝐴 𝑁𝑒
𝐸 γ
𝐼 W
=
𝐴 𝐸 γ 𝑒
𝐸 γ
𝐼 W
=
𝐴 𝑒
No w fo r t he M at h…
#
𝑐 𝑚 2 − 𝑠
Let' s s ay a gamma fl ux of Φ ̇ enters a c hamber of area A .
E ac h mak es N i on pai r s , eac h w i th a c har ge of e and ener gy W ,
an d th en s tops i n the c ham ber:
+
W ̇ = Φ ̇ 𝐸 γ
R a d i a ti o n “ I n te n s i ty ”
The abs or pti o n rate of energy i n the c ham ber i s 𝐸 ̇ 𝑎 𝑏 𝑠 = W ̇ 𝐴
Thes e c an be us ed to meas ure gamma ray energ y , pr oporti o n al to the meas ure d c urrent!
O ur Use: A Si mp le Co unt er
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Geiger tube photo courtesy of Jeff Keyzer on F lickr. – +
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Circuit diagram © Wiley-VCH, from J. Turner, Atoms, Radiation, and Radiation Protection (2007). All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/help/faq-fair-use/ .
O ur Use: A Si mp le Co unt er
P ubl i c doma i n i ma ge .
Geiger tube photo courtesy of Jeff Keyzer on F lickr.
Circuit diagram © Wiley-VCH, from J. Turner, Atoms, Radiation, and Radiation Protection (2007). All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/help/faq-fair-use/ .
W e u se cir cu it r y t o d e t e ct t h e ri s i ng edge of the pul s e from the Gei ger tube
S et s om e thres hol d to c al l the edge r ise n
Se n d t h is ( n o w d ig it a l) sig n a l t o our LE D s and the s peak er to mak e l i ght and nos e!
Circuit diagram © Wiley-VCH, from J. Turner, Atoms, Radiation, and Radiation Protection (2007). All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/help/faq-fair-use/ .
L et ’ s R e- Exami ne O ur Ci r cui t
Courtesy of Mark Chilenski. Used with permission.
That’ s our r ising edge tr igger !
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T ran si st o r i s bot h a s wit c h a nd a n inv e r t e r
555 t i mer i s t r igge r e d t o c ha r ge it s cap aci t o r ( ch arg e b u cket ) unt il f ull
L o o k Clo ser : Ri si ng Ed g e T r i g g er
Thi s si gna l i s s ent t o s pea k er s and LE Ds
Courtesy of Mark Chilenski. Used with permission. 17
O ur M easur ed W avefo r ms
Ac t ua l S BM - 20 G ei ge r t ube w av e f or m
P ul se st r et cher ( s ound and l i ght ) w av ef or m
L i mi t i ng Cases: H i g h Si g nal
N o pr oblem !
GM T ube
W hat happens if LOTS of counts com e in at once?
P uls e S t ret ch er
Missed count!
This is known as “ dead tim e,” a per iod when the detector is unr esponsi ve
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2 3 4
T rue Ev ents
Which app li es to our cas es?
t
t
P ar alyzable Detector
t
Non-P ar alyzable
Detector
P uls e S t ret ch er
P ar aly zable vs. No n- P ar aly zable
GM T ube
P ar aly zable vs. No n- P ar aly zable
Incr ease count r ate
Circuit diagram © Wiley-VCH, from J. Turner, Atoms, Radiation, and Radiation Protection (2007). All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/ help/faq-fair-use/ .
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P ar aly zable vs. No n- P ar aly zable
GM T ube
Geiger tube photo courtesy of Jeff Keyzer on F lickr.
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V ery r api d radi ati o n ev ents k eep t he i on c urrent hi gh
T h is m a in t a in s t h e cir cu it vo lt a g e abov e t he ri s i ng edge tri gger thr es hol d
The GM tube i s therefor e par alyz able , b u t it s d e a d t im e is ve r y low ( < 1 µ s)
Circuit diagram © Wiley-VCH, from J. Turner, Atoms, Radiation, and Radiation Protection (2007). All rights reserved. This content is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/help/faq-fair-use/ .
P ar aly zable vs. No n- P ar aly zable
P uls e S t ret ch er
V ery rapi d radi ati o n ev ents don' t re - t r ig g e r ca p a cit o r d isch a r g e
No a d d it io n a l t im e is sp e n t a t lo g ic h ig h vo lt a g e
The pul s e s tretc her i s t herefore non - par alyz able , b u t it s d e a d t im e is ve r y high ( ~ 1 . 5 m s)
T hi nki ng Ahead fo r t he L ab
How will you char a cter i ze GM dead tim e ?
How will you char a cter i ze pu l se str etcher dead tim e?
Wher e on your cir cuit will you connect the com puter to m easur e counts?
What other sour ces of dead tim e exist in the system ? Hint: T her e ar e som e!
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22. S902 Do-It-Yourself (DIY) Geiger Counters
January IAP 2015
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