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Table 1 Overview of the properties of the argon beam at different temperatures of the valve housing T valve, repetition rates frep (which are determined by the velocity of the stored ammonia molecules), ammonia velocities \(v_{\mathrm {ND_{3}}}\), and durations of the current pulse applied to the valve Δtpulse. The second block lists properties of the beams measured at detection zone II: the relative beam intensity, mean arrival time, 〈τ〉, the width of the arrival time distribution Δτ, and the full width at half maximum (FWHM) length of the argon packet \(L=\left \langle v_{Ar} \right \rangle \times 2 \sqrt {2\ln 2}~\Delta \tau \). Finally, the last block lists the parameters found from a simultaneous fit to the time-of-flight distributions measured at both detectors: the mean 〈vAr〉 and standard deviation \(\sigma _{v_{Ar}}\) of the velocity distribution, duration of valve opening time, and the effective distance between the valve and detection zone II

From: A detailed account of the measurements of cold collisions in a molecular synchrotron

T valve (°C)

frep (Hz)

\(v_{\mathrm {ND_{3}}}\) (m/s)

Δtpulse (μs)

rel. int.

〈τ〉 (ms)

Δτ (μs)

L (mm)

〈vAr〉 (m/s)

\(\sigma _{v_{\text {Ar}}}\) (m/s)

pw (μs)

Δz (m)

+30

153

121.1

27.3

3.00 ±0.20

2.207

96

137

570.56

24.01

22.41

1.265

 

175

138.8

 

2.74 ±0.18

2.205

94

134

571.41

24.09

22.48

1.265

−30

153

121.1

25.2

2.02 ±0.12

2.380

124

163

524.08

27.57

11.24

1.255

 

175

138.8

 

1.91 ±0.11

2.378

122

160

524.73

27.30

13.73

1.254

−90

153

121.1

23.6

1.31 ±0.11

2.604

162

192

474.51

28.48

10.00

1.245

 

175

138.8

 

1.21 ±0.10

2.597

159

189

475.40

29.22

10.00

1.245

−150

153

121.1

22.8

1.11 ±0.10

2.921

173

183

421.92

24.32

10.00

1.241

 

175

138.8

 

1.00 ±0.09

2.916

175

185

423.40

24.98

10.00

1.242