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06 - Photomultiplier Tubes and Photodiodes 06 - Photomultiplier tubes and photodiodes Jaroslav Adam Czech Technical University in Prague Version 2 Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 1 / 38 The Photomultiplier (PM) tube Detection of very weak scintillation light Provide electrical signal Can be also done with silicon photodiodes, but PM are most widely used Characterized by spectral sensitivity Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 2 / 38 Structure of PM tube Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 3 / 38 Photoemission process Conversion of incident light to photelectron in sequence of processes (1) photon absorbed, it’s energy transfered to electron in material (2) Migration of electron to the surface of material (3) Escape of electron from the surface of photocathode Must overcome potential barrier (work function) of the material Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 4 / 38 Spontaneous electron emission Thermionic noise by the surface barrier Thermal kinetic energy of conduction electrons may be sufficient to overcome the barrier Average of thermal energy is 0.025 eV, but the tail of the distribution reaches higher energies Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 5 / 38 Fabrication of photocathodes Opaque - thickness > maximal escape depth Semitransparent - deposited on transparent backing Important uniformity of thickness Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 6 / 38 Quantum efficiency and spectral response Measures sensitivity of photocathode QE = (number of photoelectrons emitted) / (number of incident photons) Depends on photon wavelength Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 7 / 38 Quantum efficiency and spectral response Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 8 / 38 Focusing the electrons from photocathode towards the first dynode RCA Photomultiplier Manual. Technical Series PT-61, 1970 Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 9 / 38 Electron multiplication Secondary electron emission Electron from photocathode accelerated towards the dynode Deposited energy cause re-emission of more secondary electrons Excited electrons within dynode, only some escape the surface Yield of secondary electrons is function of incident energy Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 10 / 38 Secondary electron emission At one dynode δ = (number of secondary electrons emitted) / (primary incident electrons) Depends on incident electron energy Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 11 / 38 Negative electron affinity Used to increase of secondary emission yield Achieved by ionized acceptors by electrons from thin electropositive surface layer Band structure bent at the surface, electron at the bottom of conduction band may escape without further energy loss Secondary emission yield shows monotonic increase with incident electron energy Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 12 / 38 Multiple stage multiplication Needed to achieve gain about 106 Second dynode attact secondary electrons emitted at low energy by first dynode Can be repeated many times gain = αδN (1) Overall gain is function of voltage Statistical broadening of response by fluctuations in multiplication Variance dominated by multiplication factor at first dynode Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 13 / 38 Structural differences of PM tubes Several configurations of photocathode and multiplier section Continuous channel electron multiplier (channeltron) Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 14 / 38 Microchannel plate Many individual tubes with small diameter Short electron transit time Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 15 / 38 Microchannel plate (MCP) in image intensifier Hamamatsu, Image intensifiers, TII 0004E02, SEPT. 2009 IP Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 16 / 38 Pulse timing properties Time characteristics of PM given by electron trajectories Electron transit time is average time difference between arrival of photon at photocathode and collection of the pulse of electrons at anode Width of pulse given by spread in transit time Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 17 / 38 Pulse timing properties Difference in electron paths dominant in spread of transit time Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 18 / 38 Spread of transit time Measured spread as a function of average number of photoelectrons per pulse Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 19 / 38 Maximum ratings Maximal voltage and current ratings Voltage between anode and cathode + photocathode and first dynode, between dynodes and last dynode and anode Current limits for photocathode and anode, of no concern in scintillator pulse counting Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 20 / 38 Photomultiplier tube specifications Overall luminous sensitivity Cathode luminous sensitivity Overall radiant sensitivity Cathode radiant sensitivity Dark current Anode pulse rise time Anode pulse width Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 21 / 38 Linearity Electron multiplication factor independent of number of original photoelectrons Output pulse amplitude linearly proportional to intensity of scintillation light Nonlinearity can be caused by space charge between last dynode and anode Demands on PM by high light yield at fast decay time of new scintillators Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 22 / 38 Noise and spurious pulses Spontaneous termionic emission of electrons from photocathode Dark spectrum of pulses from single electron: Afterpulses from ionized residual gas drifting to photocathode Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 23 / 38 Non-ideality of PM Photocathode nonuniformities Change of gain during measurement Space charge and thermal effects Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 24 / 38 High voltage supply and voltage divider Positive polarity (a), negative polarity (b) Current through divider larger than internal current of PM Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 25 / 38 Photomultiplier summary Figure : Region between photocathode and 1st dynode Figure : Typical structure (up) and negative electron affinity (down) Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 26 / 38 Photodiodes Higher quantum efficiency, compact size Insensitive to magnetic field Conventional photodiode or avalanche photodiode Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 27 / 38 Conventional photodiodes High quantum efficiency over large range of incident wavelength No internal amplification, weak output pulses Design as PIN detector Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 28 / 38 Spectral response of conventional photodiode Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 29 / 38 Avalanche photodiodes Charge multiplication in semiconductor Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 30 / 38 Silicon photomultiplier Geiger mode of avalanche photodiode Single photon sensitivity Constructed as array of small cells Number of fired cells proportional to number of scintillation photons Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 31 / 38 Scintillation pulse shape analysis Given by time constant of anode circuit: Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 32 / 38 Effect of time constant Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 33 / 38 Fluctuations in pulse shape Short time constant sensitive to fluctuations Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 34 / 38 Hybrid photomultiplier tube Electrons emitted by photocathode detected by silicon detector Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 35 / 38 Position sensing photomultiplier tubes Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 36 / 38 Metal channel dynode structure Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 37 / 38 Anode wire readout Reduction of readout channels by charge division Jaroslav Adam (CTU, Prague) DPD_06, Photomultiplier tubes and photodiodes Version 2 38 / 38.
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