iota single electron and low intensity studies
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IOTA single-electron and low-intensity studies G. Stancari for the team IOTA/FAST Group Meeting Fermilab, February 22, 2019 https://indico.fnal.gov/event/19797 Study of Thu Feb 21 (8 h) - M3L MCP-PMT signals (MCP out + 4 anodes) are good for


  1. IOTA single-electron and low-intensity studies G. Stancari for the team IOTA/FAST Group Meeting 
 Fermilab, February 22, 2019 https://indico.fnal.gov/event/19797

  2. Study of Thu Feb 21 (8 h) - M3L MCP-PMT signals (MCP out + 4 anodes) are good for timing and position down to ~uA intensities. Sensitivity does not reach single electrons, limited by noise (20 kHz, 400 kHz, 500 kHz, ...). Needs to be investigated and mitigated. Relied mostly on M2R camera intensities. - Collected data on mini-injections repeated every ~60 s. Reliably injected 0 to 3 electrons by inserting screens and regulating laser wave plate. Recorded M2R camera images of 1 stored electron. - Injected ~110 electrons and let intensity decay to study statistics of individual electron loss times and to measure beam lifetime in 10-100 pA range � 2 Giulio Stancari | IOTA low-intensity studies IOTA/FAST Group Meeting | Fermilab, 22 Feb 2019

  3. Photomultiplier signals with 0.48 mA circulating in IOTA M3L MCP-PMT out 20-50 mA noise limits sensitivity (on both Heliax M3L MCP-PMT 
 and RG-58 cables) anode 1 Needs to be filtered or mitigated M2L PMT anode 7.5-MHz marker � 3 Giulio Stancari | IOTA low-intensity studies IOTA/FAST Group Meeting | Fermilab, 22 Feb 2019

  4. Mini-injections Inserted screens in linac, tuned laser wave plate, injected every ~60 s M2R camera intensity [arb. units] 3 e - 2 e - 1 e - 0 e - 0 500 1000 1500 2000 2500 Time [s] Variation on what was done in November (no IOTA injection quad detuning). Shown reliable injection of a few electrons. Also part of our current LDRD on the feasibility of single-electron studies. � 4 Giulio Stancari | IOTA low-intensity studies IOTA/FAST Group Meeting | Fermilab, 22 Feb 2019

  5. Intensity and lifetime measurement down to microamps DCCT Two methods (to assess systematics) (1) Exponential fit M2L PMT 
 (2) Derivative of smooth spline current gain x32 gain x4.5 1 μ A 7.5 MHz M2L PMT 
 counts � 5 Giulio Stancari | IOTA low-intensity studies IOTA/FAST Group Meeting | Fermilab, 22 Feb 2019

  6. Intensity and lifetime in 1-100 pA range (in progress) Two methods (to assess systematics) (1) Exponential fit (2) Max-likelihood fit of intervals between P ( T i ) = λ exp( − λ T i ) individual electron losses (steps) � 6 Giulio Stancari | IOTA low-intensity studies IOTA/FAST Group Meeting | Fermilab, 22 Feb 2019

  7. Beam lifetime vs. intensity IOTA beam lifetime vs. intensity Data of Feb. 14, 2019, 13:30 − 16:02 ● 10 10 ● 8 ● Decay rate [%/min] ● Lifetime [min] 15 N:IBEAM (DCCT) ● ● ● 6 ● N:IBEASL (sync − light PMT) ● ● 20 ● ● ● ● ● ● 4 ● ● 30 ● ● ● ● ● ● ● 45 ● ● 2 ● ● 60 ● 120 0.005 0.010 0.020 0.050 0.100 0.200 0.500 Beam intensity [mA] � 7 Giulio Stancari | IOTA low-intensity studies IOTA/FAST Group Meeting | Fermilab, 22 Feb 2019

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