2,594,703 424-21%-4

Total Page:16

File Type:pdf, Size:1020Kb

2,594,703 424-21%-4 April 29, 1952 L. F. WOUTERs 2,594,703 PHOTOMULTIPLIER TUBE CIRCUIT Filed March 7, 195l. 62 222 34 A2 SQUARE WAVE VOLTAGE GENERATOR INVENTOR, LOUIS F WOUTERS BY 424-21%-4---- ATTORNEY. Patented Apr. 29, 1952 2,594,703 UNITED STATES PATENT OFFICE 2,594,703 PHOTOMULTIPLERTUBE CIRCUIT Louis F. Wouters, Oakland, Calif., assignor to the United States of America as represented by the United States Atomic Energy Commission Application April 17, 1951, serial No. 221,396 4 Claims. (CL 250-207) 2 This invention relates to a photomultiplier prising a plurality of similar resistors and tube circuit and more particularly to a method similar capacitors 8, is connected between the and apparatus for increasing the output of a cathode and penultimate dynode with intermedi photomultiplier tube. ate connections thereof connected to the first In many circuits utilizing photomultiplier tubes s seven dynodes, so that a resistor and a capacitor it is necessary to amplify the output of such are parallel-connected between each of such elec tubes so that they may be applied to auxiliary trodes. In the present embodiment of the inven circuits. Thus, if the source of light is faint, tion the penultimate dynode is connected directly the electron multiplication of the photomulti to ground by a lead 2 while the cathode is con plier tube may be insufficient to raise the output () nected to one side of a storage capacitor 22 by to a readily useful level requiring expensive, as a lead 23. The other side of the capacitor 22 is well as, extensive amplifier circuits. In some connected to the anode of a triode type tube 26, instances the desire to maintain the pulse shape the Cathode of which is grounded. and resolution time of the output requires addi As a means for supplying unidirectional volt tionally complex pulse forming and shaping am 5 age to the photomultiplier tube 3 there is pro plifiers. vided a conventional power supply 3. having. a The present invention provides a photomulti plurality of output voltages. For purposes of plier tube circuit which overcomes the above illustration the values of such output voltages outlined difficulties by operating the photomulti will hereinafter be numerically identified by the plier tube at voltages many times the normal op 20 voltage existing with respect to a grounded ter erating voltages for such tube. The foregoing minal 32, but should not be understood as limit is made practical by pulsed operation which pre ing the circuit to the exact voltages set forth. vents deleterious overloading of the photomulti A negative terminal 33 having a value of -100 plier tube. - volts is connected to the control grid of the tube It is therefore an object of the present inven 25 26 through a biasing resistor 36. A positive 'ter tion to provide a new and improved photomulti minal 35 having a value of -2000 voltS. is con plier tube circuit. nected through a dropping resistor 36 to the Another object of the invention is to provide anode of the tube 26 to supply operating voltage a photomultiplier tube circuit which may di thereto and also a charging voltage to the rectly drive an auxiliary circuit. 30 capacitor 22. A second positive terminal 37 Still another object of the invention is to having a value of -250 volts is connected to provide a photomultiplier tube circuit having a the final dynode of the tube 3 to Supply a Suit pulsed power supply therefor to provide greater able operating potential thereto through a drop amplification through such tube. ping resistor 38. A third positive terminal 39 A further object of the invention is to provide 35 having a value of --500 volts is connected to a photomultiplier tube circuit which is simple in the anode of the tube 13 through a dropping construction and which eliminates the necessity resistor 40 to supply a suitable operating poten of amplifiers in the output circuit. - tial thereto. ... Still further objects and advantages of the It will be seen that with the power supply 3 invention will be apparent from the following 40 suitably energized that the capacitor 22 will be description and claims considered together with come charged to the value of the power Supply the accompanying drawing which is a schematic terminal 35, that is --2000 volts, but that the side wiring diagram. - of the capacitor connected to the cathode of the Referring to the drawing in detail there is tube 3 is at ground potential. Now, if the posi provided a source of light, Such as a Scintilla 45 tively charged side of the capacitor 22 is Sud tion crystal f, placed in the path of a beam of denly connected to ground, the voltage of the charged particles 2. Disposed adjacent the cathode of the tube 3 will be effectively lowered crystal it is a photomultiplier tube f3 in Such to a value of -2000 volts which will be evenly position that light from the crystal falls upon distributed across the resistors f to ground, the light-sensitive cathode of the tube. The 50 Thus the photomultiplier tube 3 will be opera photomultiplier tube 3, as illustrated in the tive to pass electrons between the cathode and drawing, has nine dynodes disposed between the. anode by way of the dynodes upon activation of cathode and anode and it will be readily ap the cathode by light striking thereon. To ac parent that other types of photomultiplier tubes complish Such mode of operation a Square Wave may be substituted. A voltage divider 6, com 55 voltage generator 46 of conventional design and 2,594,708 3 4 having an output sufficient to overcome the the other side of the resistor 52 by the capacitor negative grid bias of the tube 26 is connected 57 the unidirectional voltages at such electrodes between the control grid and cathode thereof. are blocked and only the varying voltage caused The duration of the square wave output of the by the electron flow is passed. Such varying generator 46 should be short as compared to the voltage establishes a push-pull voltage across the time constant of the capacitor 22 and the re resistor 52 and thereby causes deflection of the sistance of the resistors so that the high Volt electron beam of the oscilloscope 59. Thus a age across the elements of the photomultiplier pattern of the magnitude and duration of the tube will not be damaged by prolonged over light scintillation at the crystal is formed on voltage. The repetition rate of the generator 46 O the Screen of the Oscilloscope 59. is not critical, but should be sufficiently rapid to From the foregoing it will be readily apparent energize the circuit for each Scintillation of the that any desired light source may be utilized in crystal in the present embodiment of the in the position of the crystal . It will also be vention and still have an average value which readily understood that numerous types of loads is not in excess of the voltage rating of the may be connected to the output of the photo tube f3. multiplier tube to be driven thereby, in the place The output of the photomultiplier tube 3 may of the OScilloscope 59. be taken from between the final dynode and While the salient features of this invention anode thereof and will be of sufficient magnitude have been described in detail with respect to one to directly drive an auxiliary circuit. As illus 20 embodiment it will, of course, be understood that trated in the drawing a lead 5 is connected to numerous modifications may be made within the the final dynode of the tube 3 and coupled to Spirit and Scope of the invention and it is there one end of a center-grounded resistor 52 by a ca fore not desired to limit the invention to the exact pacitor 53. A lead 56 is similarly connected to details shown except insofar as they may be de the anode of the tube 3 and coupled to the other ; fined in the following claims. end of the resistor 52 by a capacitor 57. Thus a What is claimed is: push-pull voltage is developed across the re 1. In a photomultiplier tube circuit, the comi sistor 52 which may then be impressed between bination comprising a source of light, a photo the vertical deflecting plates of an oscilloscope multiplier tube having an anode, a plurality of 59. The oscilloscope 59 is equipped with a power dynodes, and a cathode with substantially low Supply 6 to energize the electron gun and to values of operating voltages, said tube being dis energize the Sweep generator 62 which is in turn posed adjacent Said source to receive light there connected to the horizontal deflecting plates. from, a voltage divider having a plurality of Now consider the operation of the present in equally Spaced taps connected between the penul wention, as described above, with the power Sup timate dynode and said cathode with the taps plies 3 and 6 and the square wave generator respectively connected to the dynodes, said penul 46 suitably energized. Under such condition a timate dynode being connected to ground, said Square Wave of voltage at the output of the gen cathode being connected to a storage capacitor, erator 46 renders the triode tube 26 conductive power supply means having a grounded terminal, to ground the positively charged side of the a positive terminal connected to said capacitor capacitor 22. Thus the cathode of the photo for charging the capacitor to a high value of multiplier tube f3 is biased to -2000 volts.
Recommended publications
  • Building a Photomultiplier Tube Testing Lab and Measuring Dark Rate
    Building a photomultiplier tube testing lab and measuring dark rate Suffolk County Community College and Brookhaven National Lab Lab Setup • Dark box set up to hold four Photomultiplier tubes simultaneously and output signals • Three step data collection 1. Discriminator 2. Delay Generator 3. Visual Scalar • Labview collects and files data and Oscilloscope shows signal outputs from PMTs Wiring Discriminator: The PMTs constantly output a signal (Dark current) regardless of whether or not it detected a photon. The discriminator sets a voltage that has to be exceeded for the signal to pass through. Delay Generator: The delay generator receives the input from the discriminator and outputs to the visual scalar. When active, the delay generator allows the signal to pass through, but only for a set period of time. Visual Scalar: The visual scalar receives the output from the delay generator and outputs the number of signals it receives. Dark Box “light tight” testing • The first problem we encountered with the dark box was there was there was a measureable difference in counts when testing with the lights on vs. the lights off. This meant that the box wasn’t completely sealed • We taped any visible weaknesses in the box and added a layer of foam tape between the box and the lid • We tested the modified box at several different voltages with the lights both on and off and the differences were negligible • The data is plotted above, the red line represents the data collected with the lights on and the black line represents the data with the lights off Dark Current • PMTs constantly output a very low signal whether or not the have detected a photon.
    [Show full text]
  • Characterisation of Silicon Photomultipliers for the Detection of Near Ultraviolet and Visible Light
    Universit`adegli Studi di Trento { Dipartimento di Fisica Fondazione Bruno Kessler { Integrated Radiation and Image Sensors Characterisation of Silicon Photomultipliers for the detection of Near Ultraviolet and Visible light Cycle XXIX G. Zappala' Supervised by: N. Zorzi Abstract Light measurements are widely used in physics experiments and medical ap- plications. It is possible to find many of them in High{Energy Physics, As- trophysics and Astroparticle Physics experiments and in the PET or SPECT medical techniques. Two different types of light detectors are usually used: thermal detectors and photoelectric effect based detectors. Among the first type detectors, the Bolometer is the most widely used and developed. Its in- vention dates back in the nineteenth century. It represents a good choice to detect optical power in far infrared and microwave wavelength regions but it does not have single photon detection capability. It is usually used in the rare events Physics experiments. Among the photoelectric effect based detectors, the Photomultiplier Tube (PMT) is the most important nowadays for the de- tection of low{level light flux. It was invented in the late thirties and it has the single photon detection capability and a good quantum efficiency (QE) in the near{ultraviolet (NUV) and visible regions. Its drawbacks are the high bias voltage requirement, the difficulty to employ it in strong magnetic field environments and its fragility. Other widely used light detectors are the Solid{State detectors, in particular the silicon based ones. They were developed in the last sixty years to become a good alternative to the PMTs. The silicon photodetectors can be divided into three types depending on the operational bias voltage and, as a conse- quence, their internal gain: photodiodes, avalanche photodiodes (APDs) and Geiger{mode detectors, Single Photon Avalanche Diodes (SPADs).
    [Show full text]
  • Pentodes Connected As Triodes
    Pentodes connected as Triodes by Tom Schlangen Pentodes connected as Triodes About the author Tom Schlangen Born 1962 in Cologne / Germany Studied mechanical engineering at RWTH Aachen / Germany Employments as „safety engineering“ specialist and CIO / IT-head in middle-sized companies, now owning and running an IT- consultant business aimed at middle-sized companies Hobby: Electron valve technology in audio Private homepage: www.tubes.mynetcologne.de Private email address: [email protected] Tom Schlangen – ETF 06 2 Pentodes connected as Triodes Reasons for connecting and using pentodes as triodes Why using pentodes as triodes at all? many pentodes, especially small signal radio/TV ones, are still available from huge stock cheap as dirt, because nobody cares about them (especially “TV”-valves), some of them, connected as triodes, can rival even the best real triodes for linearity, some of them, connected as triodes, show interesting characteristics regarding µ, gm and anode resistance, that have no expression among readily available “real” triodes, because it is fun to try and find out. Tom Schlangen – ETF 06 3 Pentodes connected as Triodes How to make a triode out of a tetrode or pentode again? Or, what to do with the “superfluous” grids? All additional grids serve a certain purpose and function – they were added to a basic triode system to improve the system behaviour in certain ways, for example efficiency. We must “disable” the functions of those additional grids in a defined and controlled manner to regain triode characteristics. Just letting them “dangle in vacuum unconnected” will not work – they would charge up uncontrolled in the electron stream, leading to unpredictable behaviour.
    [Show full text]
  • Eimac Care and Feeding of Tubes Part 3
    SECTION 3 ELECTRICAL DESIGN CONSIDERATIONS 3.1 CLASS OF OPERATION Most power grid tubes used in AF or RF amplifiers can be operated over a wide range of grid bias voltage (or in the case of grounded grid configuration, cathode bias voltage) as determined by specific performance requirements such as gain, linearity and efficiency. Changes in the bias voltage will vary the conduction angle (that being the portion of the 360° cycle of varying anode voltage during which anode current flows.) A useful system has been developed that identifies several common conditions of bias voltage (and resulting anode current conduction angle). The classifications thus assigned allow one to easily differentiate between the various operating conditions. Class A is generally considered to define a conduction angle of 360°, class B is a conduction angle of 180°, with class C less than 180° conduction angle. Class AB defines operation in the range between 180° and 360° of conduction. This class is further defined by using subscripts 1 and 2. Class AB1 has no grid current flow and class AB2 has some grid current flow during the anode conduction angle. Example Class AB2 operation - denotes an anode current conduction angle of 180° to 360° degrees and that grid current is flowing. The class of operation has nothing to do with whether a tube is grid- driven or cathode-driven. The magnitude of the grid bias voltage establishes the class of operation; the amount of drive voltage applied to the tube determines the actual conduction angle. The anode current conduction angle will determine to a great extent the overall anode efficiency.
    [Show full text]
  • The Venerable Triode
    The Venerable Triode The very first gain device, the vacuum tube Triode, is still made after more than a hundred years, and while it has been largely replaced by other tubes and the many transistor types, it still remains popular in special industry and audio applications. I have some thoughts on why the Triode remains special for audio amplifiers (apart from sentimental value) that I would like to share. But first, a quick tutorial about Triodes: The earliest Triode was Lee De Forest's 1906 “Audion”. Over a hundred years development has resulted in many Triodes, large and small. The basic design has remained much the same. An evacuated container, usually glass, holds three signal connections, seen in the drawing as the Cathode, Grid and Plate (the Plate is also referred to as the Anode). In addition you see an internal heater, similar to a light bulb filament, which is used to heat the Cathode. Triode operation is simple. Electrons have what's known as “negative electrostatic charge”, and it is understood that “like” charges physically repel each other while opposite charges attract. The Plate is positively charged relative to the Cathode by a battery or other voltage source, and the electrons in the Cathode are attracted to the Plate, but are prevented by a natural tendency to hang out inside the Cathode and avoid the vacuum. This is where the heater comes in. When you make the Cathode very hot, these electrons start jumping around, and many of them have enough energy to leave the surface of the Cathode.
    [Show full text]
  • Photomultiplier Tubes 1)-5)
    CHAPTER 2 BASIC PRINCIPLES OF PHOTOMULTIPLIER TUBES 1)-5) A photomultiplier tube is a vacuum tube consisting of an input window, a photocathode, focusing electrodes, an electron multiplier and an anode usu- ally sealed into an evacuated glass tube. Figure 2-1 shows the schematic construction of a photomultiplier tube. FOCUSING ELECTRODE SECONDARY ELECTRON LAST DYNODE STEM PIN VACUUM (~10P-4) DIRECTION e- OF LIGHT FACEPLATE STEM ELECTRON MULTIPLIER ANODE (DYNODES) PHOTOCATHODE THBV3_0201EA Figure 2-1: Construction of a photomultiplier tube Light which enters a photomultiplier tube is detected and produces an output signal through the following processes. (1) Light passes through the input window. (2) Light excites the electrons in the photocathode so that photoelec- trons are emitted into the vacuum (external photoelectric effect). (3) Photoelectrons are accelerated and focused by the focusing elec- trode onto the first dynode where they are multiplied by means of secondary electron emission. This secondary emission is repeated at each of the successive dynodes. (4) The multiplied secondary electrons emitted from the last dynode are finally collected by the anode. This chapter describes the principles of photoelectron emission, electron tra- jectory, and the design and function of electron multipliers. The electron multi- pliers used for photomultiplier tubes are classified into two types: normal dis- crete dynodes consisting of multiple stages and continuous dynodes such as mi- crochannel plates. Since both types of dynodes differ considerably in operating principle, photomultiplier tubes using microchannel plates (MCP-PMTs) are separately described in Chapter 10. Furthermore, electron multipliers for vari- ous particle beams and ion detectors are discussed in Chapter 12.
    [Show full text]
  • Precise Db Monitoring with Eye Tubes This Circuit for Use with Eye Tubes Eliminates Variations for Precise and Accurate Signal Measurements
    tubes Precise dB Monitoring with Eye Tubes This circuit for use with eye tubes eliminates variations for precise and accurate signal measurements. By Joe Sousa uning eye, or indicator, tubes came into use before World War II to help tune radio re- ceivers by indicating signal strength. This was helpful to reduce Tdistortion and adjacent channel inter- ference that would result if the radio were tuned too far from the center of the channel. The eye tubes were de- veloped as a cheaper alternative to the needle movement meters. It was not until the 1960s that needle meters were made economically enough in Japan to displace indicator tubes. During the decades from the 1930s to PHOTO 1: EM84/6FG6 with triode grid input at 0V, –3V, and –23V. the 1960s, when tuning indicator tubes were in production, they found wide use of the tube. The green rectangles grow to deflect the output beam on the fluo- in instrumentation as a low-cost alterna- longitudinally, as the input signal grows rescent target painted on the side of the tive to the needle meter. Capacitor mea- more negative (Photo 1). At full signal glass envelope. The 470k plate resistor surement bridges and tube testers were strength, the two among the more common instruments rectangles meet in making use of these inexpensive indica- the center, form- tor tubes. ing a solid rect- By the 1950s, indicator tube design angle 1.5˝ long. had matured enough that good preci- Figure 1 shows sion could be obtained for use as re- the internal ar- cording level meters in open-reel tape rangement of the recorders.
    [Show full text]
  • Photosensitive Camera Tubes and Devices Handbook
    11.2 PHOTOSENSITIVE CAMERA TUBES AND DEVICES 11.1 PHOTOSENSITIVITY / 11.2 11.1.1 Photoemitters / 11.2 11.1.2 Photoconductors / 11.5 11.2 PHOTOELECTRIC-INDUCED TELEVISION SIGNAL GENERATION / 11.5 11.2.1 Photoemission-Induced Charge Images / 11.5 11.2.2 Secondary-Emission-Induced Charge Images / 11.6 11.2.3 Electron-Bombardment-Induced Conductivity / 11.8 11.2.4 Photoconductive-Generated Charge Images / 11.9 11.2.5 Generation of Video Signals by Scanning / 11.11 11.2.6 Low-Velocity Scanning / 11.11 11.2.7 Return-Beam Signal Generation / 11.13 11.2.8 High-Velecity Scanning / 11.14 11.3 EVOLUTION AND DEVELOPMENT OF TELEVISION CAMERA TUBES / 11.14 11.3.1 Nonstorage Tubes / 11.14 11.3.2 Storage Tubes / 11.15 11.4 VIDICON-TYPE CAMERA TUBES / 11.26 11.4.1 Antimony Trisulfide Photoconductor / 11.26 11.4.2 Lead Oxide Photoconductor / 11.28 11.4.3 Selenium Photoconductor / 11.30 11.4.4 Silicon-Diode Photoconductive Target / 11.31 11.4.5 Cadmium Selenide Photoconductor / 11.32 11.4.6 Zinc Selenide Photoconductor / 11.32 11.5 INTERFACE WITH THE CAMERA / 11.33 11.5.1 Optical Input / 11.34 11.5.2 Operating Voltages / 11.34 11.5.3 Dynamic Focusing / 11.36 11.5.4 Beam Blanking / 11.36 11.5.5 Beam Trajectory Control / 11.38 11.5.6 Video Output / 11.40 11.5.7 Deflecting Coils and Circuits / 11.42 11.5.8 Magnetic Shielding / 11.42 11.5.9 Anti-Comet-Tail Tube / 11.42 11.6 CAMERA TUBE PERFORMANCE CHARACTERISTICS / 11.43 11.6.1 Sensitivity and Output / 11.44 11.6.2 Resolution / 11.45 11.6.3 Lag / 11.49 11.6.4 Lag-Reduction Techniques / 11.50 11.7 SINGLE-TUBE COLOR CAMERA SYSTEMS / 11.54 11.7.1 Single-Output-Signal Tubes / 11.55 11.7.2 Multiple-Output-Signal Tubes / 11.58 11.8 SOLID-STATE IMAGER DEVELOPMENT / 11.60 11.8.1 Early Imager Devices / 11.60 11.8.2 Improvements in Signal-to-Noise Ratio / 11.60 11.8.3 CCD Structures / 11.61 11.8.4 New Developments / 11.63 REFERENCES / 11.64 PHOTOSENSITIVITY 11.3 11.1 PHOTOSENSITIVITY A photosensitive camera tube is the light-sensitive device utilized in a television camera to develop the video signal.
    [Show full text]
  • 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,
    [Show full text]
  • An Improved Design of the Readout Base Board of the Photomultiplier Tube for Future Pandax Dark Matter Experiments
    Prepared for submission to JINST An improved design of the readout base board of the photomultiplier tube for future PandaX dark matter experiments Qibin Zheng,0,2 Yanlin Huang,0 Di Huang,1 Jianglai Liu,1,3 Xiangxiang Ren,4 Anqing Wang,4 Meng Wang,4 Jijun Yang,1 Binbin Yan,1 Yong Yang1 0Institute of Biomedical Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China 1INPAC, Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai Laboratory for Particle Physics and Cosmology, Shanghai 200240, China 2Terahertz Technology Innovation Research Institute, University of Shanghai for Science and Technology, Shanghai 200093, China 3Tsung-Dao Lee Institute, Shanghai Jiaotong University, Shanghai, 200240, China 4School of Physics and Key Laboratory of Particle Physics and ParticleIrradiation (MOE), Shandong University, Jinan 250100, China E-mail: [email protected] Abstract: The PandaX project consists of a series of xenon-based experiments that are used to search for dark matter (DM) particles and to study the fundamental properties of neutrinos. The next DM experiment PandaX-4T will be using 4 ton liquid xenon in the sensitive volume, which is nearly a factor of seven larger than that of the previous experiment PandaX-II. Due to the increasing target mass, the sensitivity of searching for both DM and neutrinoless double-beta decay (0aVV) signals in the same detector will be significantly improved. However, the typical energy of interest for 0aVV signals is at the MeV scale, which is much higher than that of most popular DM signals. In the baseline readout scheme of the photomultiplier tubes (PMTs), the dynamic range is very limited.
    [Show full text]
  • Photomultiplier Tube Basics Photomultiplier Tube Basics
    Photomultiplier tube basics Photomultiplier tube basics Still setting the standard 8 Figures of merit 18 Single-electron resolution (SER) 18 Construction & operating principle 8 Signal-to-noise ratio 18 The photocathode 9 Timing 18 Quantum efficiency (%) 9 Response pulse width 18 Cathode radiant sensitivity (mA/W) 9 Rise time 18 Spectral response 9 Transit-time and transit-time differences 19 Transit-time spread, time resolution 19 Collection efficiency 11 Very-fast tubes 11 Linearity 19 Fast tubes 11 External factors affecting linearity 19 General-purpose tubes 11 Internal factors affecting linearity 20 Tubes optimized for PHR 12 Linearity measurement 21 Measuring collection efficiency 12 Stability 21 The electron multiplier 12 Long-term drift 21 Secondary emitting dynode coatings 13 Short-term shift (or count rate stability) 22 Voltage dividers 13 Gain 1 Supply and voltage dividers 23 Anode collection space 1 Applying the voltage 23 Anode sensitivity 1 Voltage dividers 2 Specifications and testing 1 Anode resistor 2 Maximum voltage ratings 1 Gain adjustment 2 Anode dark current & dark noise 1 Magnetic fields 2 Ohmic leakage 1 Thermionic emission 1 Magnetic shielding 27 Field emission 1 Environmental considerations 28 Radioactivity 1 Temperature 28 PMT without scintillator 1 Atmosphere 29 PMT with scintillator 1 Mechanical stress 29 Cathode excitation 1 Radiation 29 Dark current values on test tickets 1 Reference 30 Afterpulses 17 www.photonis.com Still setting Construction the standard & operating principle A photomultiplier tube is
    [Show full text]
  • Unusual Tubes
    Unusual Tubes Tom Duncan, KG4CUY March 8, 2019 Tubes On Hand GAS-FILLED HIGH-VACUUM • Neon Lamp (NE-51) • Photomultiplier • Cold-cathode Voltage (931A) Regulator (0B2) • Magic Eye (1629) • Hot-cathode Thyratron • Low-voltage (12DY8) (884) • Space Charge (12K5) 2 Timeline of Related Events 1876, 1902 William Crookes Cathode Rays, Glow Discharge 1887 [1921] Hertz, Einstein Photoelectric Effect 1897 [1906] J. J. Thomson Electron identified 1920 Daniel Moore (GE) Voltage Regulator 1923 Joseph Slepian Secondary Emission (Westinghouse) 1928 Albert Hull, Irving Thyratron Langmuir (GE) [1928] Owen Richardson Thermionic Emission 1936 Vladimir Zworykin Photomultiplier (RCA) 1937 Allen DuMont Magic Eye 3 Neon Bulbs • Based on glow-discharge (coronal discharge) effect noticed by William Crookes around 1902. • Exhibit a negative incremental resistance over part of the operating range. • Light-sensitive: photo-ionization causes the ionization voltage to decrease with illumination (not generally a desirable characteristic). • Used as indicators , voltage regulators, relaxation oscillators , and the larger ones for illumination . 4 Neon Lamp/VR Tube Curves 80 Normal Abnormal Glow Glow 70 60 Townsend Discharge 50 Negative Resistance 40 Region 30 Volts across Device across Volts 20 10 Conduction Destroys Lamp Destroys Arc Conduction Arc Chart details (coronal) Glow depend on -5 element 10 -20 10 -15 10 -10 10 1 geometry and Current through Device (A) gas mixture. 5 Cold-Cathode Voltage Regulator Tubes • Very similar to neon bulbs: attention paid to increasing current-carrying capability and ensuring a constant forward voltage. • Gas sometimes includes radio-isotopes to reduce sensitivity to photo-ionization. • Developed at General Electric Research Labs by Daniel Moore around 1920.
    [Show full text]