PMT Base for Shashlik

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    PMT base for Shashlik:

    Advance Report(why did it take so long)

    Alam Toro

    Juan Ignacio VegaRen Ros

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    Index

    Part 1: PMT base design considerations

    Part 2: PMT base test

    Part 3: Connecting R3998-02 to the base Part 4: Proposal on possible failures

    Part 5: Results

    Part 6: Conclusions

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    PMT base design considerations

    Based on Sergey calculations, a current of 0.4[A] isestimated to be the output current from PMT attached tothe Shashlik Calorimeter. To operate in this way, a gain of3x105 is needed.

    Under this considerations, a current of at least 100 timesthe PMT output is needed to be provided by the resistivenetwork, in order to dont change dynodes potentials andconsequently the PMT gain. We selected a value of currenta little bit bigger to make easier the resistance selection.

    We cannot choose a big current, because a very smallpower dissipation is needed. In this way we dont perturbthe PMT with heat coming from the resistors.

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    PMT base design considerations

    Selected current:

    100[A]

    Gain:

    3x105

    Voltage:

    820[V]

    Total Resistance:

    8.2[M]

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    PMT base design considerations

    This is normal voltage

    distribution ratio,

    found in Hamamatsu

    R3998-02 datasheet.

    Also we can find a

    suitable base made byHamamatsu

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    PMT base design considerations

    But in order to improve output linearity, is better to use a

    tapered network.

    In R3998-02 datasheet there

    wasnt a proposed tapered

    network, so Sergey suggested

    to use the following one:

    K G D1 D2 D3 D4 D5 D6 D7 D8 D9 P

    3 1 1 1 1 1 1.5 1 1 1.5 2.5

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    PMT base design considerations

    Finally the desired network was the following

    one:

    10 K output impedance was selected (bigger output signal, but damping may

    appear if connected to 50 equipment). 1K isolation was used between

    HVground and HFground (with optional capacitor too). Also additional HVsupplies are used for last dynodes.

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    PMT base test

    Before 510K resistance arrived to UTFSM, we

    made some prototypes using a 470K

    resistance, very close to the desired value.

    Voltage measurements were done and we

    found that even though we had a little

    discrepancy between measured and predicted

    voltages, the base was good enough to workproperly.

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    PMT base test base 1 200 Vsupply

    200

    Resistance [MOhm] Theorics Voltages Measured Voltages Relative Error

    0,22 5,633802817 8,9 58,0%

    1,5 38,41229193 33,6 12,5%

    0,47 12,03585147 11,66 3,1%

    0,47 12,03585147 11,68 3,0%0,47 12,03585147 11,56 4,0%

    0,47 12,03585147 11,62 3,5%

    0,47 12,03585147 11,64 3,3%

    0,75 19,20614597 18,32 4,6%

    0,47 12,03585147 11,66 3,1%

    0,47 12,03585147 11,66 3,1%

    0,75 19,20614597 18,3 4,7%

    1,3 33,29065301 30 9,9%

    sums 7,81 200 190,6

    * this voltage couldn't be measured directly due to base design

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    PMT base test base 2 1000 Vsupply

    1000

    Resistance [MOhm] Theoric Voltages Measured Voltages Relative Error

    Measured

    Resistance Resistance Error

    0,22 28,16901408 45 59,8% 0,217 1,36%

    1,5 192,0614597 167,5 12,8% 1,444 3,73%

    0,47 60,17925736 58,2 3,3% 0,468 0,43%0,47 60,17925736 58,2 3,3% 0,467 0,64%

    0,47 60,17925736 57,6 4,3% 0,464 1,28%

    0,47 60,17925736 57,9 3,8% 0,465 1,06%

    0,47 60,17925736 58,1 3,5% 0,467 0,64%

    0,75 96,03072983 91,2 5,0% 0,75 0,00%

    0,47 60,17925736 58,1 3,5% 0,467 0,64%

    0,47 60,17925736 58,1 3,5% 0,466 0,85%

    0,75 96,03072983 91,2 5,0% 0,752 0,27%

    1,3 166,453265 149,9 9,9% 1,281 1,46%

    7,81 1000 951

    * this voltage couldn't be measured directly due to base design

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    PMT base test

    Until that moment all measurements

    seemed to be correct, so we thoughtimmediately about connecting the

    R3998-02 PMT.

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    Connecting R3998-02 to the base

    The first thing that we were looking at

    while connecting the polarized base to

    the tube into the dark box was the onephotoelectron signal.

    We couldn't find it.

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    Connecting R3998-02 to the base

    So in order to compare signals and to see if we

    could get at least a small signal, we used a LEDsetup to work with the PMT.

    Besides that, we connected a russian PMT (87)

    in the same place to be excited by the LED.

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    Connecting R3998-02 to the base

    When we connected the Russian PMT to 1KV, with 50 impedance

    input in oscilloscope, we could see a signal coming out from

    Russian PMT. (Blue is PMT output, Violet is LED input signal).

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    Connecting R3998-02 to the base

    Russian PMT 87 resistor network

    Its the same type of divider.

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    Connecting R3998-02 to the base

    Russian

    PMT

    datasheet

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    Connecting R3998-02 to the base

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    Connecting R3998-02 to the base

    Signal in PMT due to LED is very

    large, because the LED generates

    a very big amount of light. This

    of course is not good for PMTgain, because dynodes voltages

    vary a lot, so after a short big

    peak, signal goes down fast.

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    Connecting R3998-02 to the base

    When we connected the Hamamatsu PMT polarized

    to 1.2kV to the oscilloscope at 50 input impedance,we couldnt see any signal again.

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    Connecting R3998-02 to the baseNormally PMT works perfectly well connected to a 50 impedance

    input. If we remember that cable impedance is 50 too, we get

    smaller signal damping in this case, and almost no damping if PMT

    has also 50 output impedance.

    But we have to remember that PMT output is a current pulse. Thismeans that it will go through the way that shows smaller resistance.

    Signals that we can see in the oscilloscope are voltage signals, so in

    the case of using 50 input impedance, a big amount of current will

    go directly to the oscilloscope, and voltage signal in the output PMTresistor will be small. If we use 1M input in the oscilloscope, almost

    all the current will go through the PMT output resistor, and we will

    have a bigger signal, but more damping as I explained before.

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    Connecting R3998-02 to the base

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    Because we were curious about this, we changed scope impedance

    to 1M, and we could see a very small signal (russian in blue,hamamatsu in yellow)

    Connecting R3998-02 to the base

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    Connecting R3998-02 to the base

    We couldnt explain this at the moment, but we

    thought it might be explained by a small PMTgain.

    So we tried to make the russian PMT to behave

    in the same way that Hamamatsu.

    In order to do this, we had to change russian

    PMT supply to 525[V].

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    Connecting R3998-02 to the base

    In this way both Hamamatsu and Russian PMT behave almost

    exactly in the same way. Hamamatsu in yellow, russian in green.

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    Connecting R3998-02 to the base

    1 Photoelectron signal at 1.2

    kV

    Very small1Photoelectron

    signal at 1 kV

    NO 1 Photoelectron signal can

    be seen at 963 V. Its only

    noise.

    So russian pmt behaves as

    Hamamatsu for small voltages.

    Its a gain problem!

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    Proposal on possible failures

    First guess about possible errorwas about resistance distributionratio. Hamamatsu PMT has a grid,and NO information about asuitable tapered network wasgiven by Hamamatsu. So I thought

    that gain might be small because itwasnt a good idea to make atapered network for this PMT.

    Normally, as seen for R7525 PMTgraphic at the right (the first optionto be use for Shashlik), taperednetworks have smaller gain.

    I made the change, check the newbase, made measurements, but NOSIGNIFICANT CHANGE IN SIGNALAPPEARED.

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    Proposal on possible failures

    In that moment I was withno ideas in my mind until Iremember I had noticedsomething important in the

    current given by the HighVoltage Supply.

    At 1.2kV applied toHamamatsu base (with PMT

    connected) we should have153A, but sourcemeasured 218A. Why?

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    Proposal on possible failures

    So in that moment I tookthe PMT and noticedsomething reallyimportant:

    All PMT pins were actuallyconnected to some placein the PMT (none wasunconnected but the

    short pin).Even those which werentconnected to a specificdynode.

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    Proposal on possible failures

    Base pins were in this waynamed in datasheet. WhatIC actually means isInternal Connection.

    We used those pins

    connections in PCB tobypass some voltages. Andthere was a problem withthis, because we actually

    welded all female pins inthe socket to the PCB base.

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    Proposal on possible failuresSo actually THIS was

    the problem, because

    this made a SHORT

    CIRCUIT between

    some of the dynodes

    (D3 and D5, bypassing

    D4). Current wentthrough this wire and

    not through some of

    the resistors. This

    made those dynodes(D3 to D5) to be at the

    same potential, with a

    big lack of gain.

    To repair this,

    we removed

    those pins from

    socket, so PMT

    is not

    connected

    anymore to thecircuit through

    Pin 4 and Pin 11

    (which are

    internallyconnected the

    one with the

    other inside the

    PMT).

    PIN 4PIN 11

    Connection between pins

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    Results

    Now we get a very big signal at 1M input impedance with the LED.

    (Hamamatsu in yellow, russian in blue)

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    Results

    To answer Will question, I measured russian PMT signal at 1.2 kV

    (same than before), and 1 [V/div] in 1M scope input (same scale than

    Hamamatsu in previous slide). A lot of damping is appreciated.

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    Results This is normal because it is due to BIG level of light. Also if we turn off the

    LED we still get signal, from a small amount of photons.

    1.2 kV supply. Dark box without

    LED blinking.

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    Results

    1 photoelectron signal

    at 1.2 kV

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    Results

    1 photoelectron signal at 1 kV

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    Results

    Several photoelectron signal at 1 kV

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    Conclusions

    PMT base design is ready and working.

    We have bases, so we can start manufacturing

    them today (we already started).