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3 Example Experiment 

 

The paramagnetic signal in liquid n-hexane is difficult to observe because the 
muonium polarisation is found to decay on a microsecond time scale, which is further 
reduced by the presence of dissolved oxygen.  A series of commissioning experiments 
were carried out using n-hexane in order to gauge the ability of the liquid handling rig 
to degas the liquid. 
 
This experiment was carried out using a detachable liquid-sample cell. 
 
At the start of the experiment, 100 ml of n-hexane was loaded into Vessel 1 and 
frozen to allow the removal of any dissolved gases.  An inert atmosphere of helium 
gas was introduced and the liquid subjected to four freeze-pump-thaw cycles using the 
procedures outlined above.  The sample cell was attached to one of the sample 
delivery tubes and pumped for 1 hr.  Using the vacuum created in the cell, a small 
amount of n-hexane, enough to fill the cell, was transferred.  To avoid contamination 
of the cleaned liquid, excess n-hexane was transferred to Vessel 3. 
 
After filling, the sample cell was sealed and detached from the rig.  Muon spin 
resonance experiments were performed at 2 G and 20 G followed by reattached to the 
rig.  At this point, the rig was open to the air and so had to be evacuated and pumped 
for 30 minutes.  The n-hexane held in the sample cell was transferred to Vessel 2 by 
freezing the vessel and allowing the vacuum to draw the n-hexane out of the cell.  
Gentle heating ensured that all the n-hexane was recovered. 
 
Two further sets of freeze-pump-thaw cycles resulted in samples for muon study after 
7 and 10 cycles had been performed on the clean n-hexane held in Vessel 1. 
 
The signal due to the paramagnetic species in n-hexane after each set freeze-pump-
thaw cycles is shown in Figure 1.  The fitted parameters for the diamagnetic, 
paramagnetic and missing fraction percentage along with the relaxation rate for the 
paramagnetic signal are shown in Table 1. 
 

Table 1

 Effect of successive freeze-pump-thaw cycles on the initial asymmetry 

attributable to the diamagnetic, paramagnetic and missing fractions and muonium 
relaxation rate. 

Initial asymmetry (%) 

Experiment 

Diamagnetic Paramagnetic  Missing 

Relaxation 

Rate (

µ

s

-1

  4 fpt cycles 

12.87 

3.41 

6.72 

7.96 

  7 fpt cycles 

12.41 

5.86 

4.73 

6.66 

10 fpt cycles 

12.86 

4.90 

5.24 

5.45 

 

 

 

 

 

  6 fpt cycles    
sodium dried 

12.59 4.39 6.02 5.20 

 

 
 

 

 - 

13 

Содержание Muon Liquid Handling System None

Страница 1: ...Muon Liquid Handling System User Guide C Johnson S P Cottrell et al Version 0 2 1...

Страница 2: ...essel 2 7 2 2 3 Removing air from Vessel 3 7 2 2 4 Evacuation of the sample cell 7 2 3 Freeze Pump Thaw cycle 8 2 3 1 Sample in Vessel 1 8 2 3 2 Sample in Vessel 2 8 2 3 3 Sample in Vessel 3 9 2 4 Liq...

Страница 3: ...uid handling system are shown in Figure 1 Inlet 1 Inlet 2 Gas pressure Cell pressure To pump To cell Baratron Vessel 2 Vessel 1 Vessel 3 Figure 1 The layout of the front panel on the muon liquid handl...

Страница 4: ...e a means of flowing liquid into and out of the cell along with feed throughs for an RF excitation signal and a pick up coil Figure 2 The liquid sample cell mounted on a sample stick with a flat coil...

Страница 5: ...Roughing Turbo switch Off Run switch Pressure reading Turbo control panel Turbo Pump Rotary Pump Figure 2 The layout of the front panel on the vacuum pump used with the muon liquid handling system 5...

Страница 6: ...ls It is important to note that a small amount of liquid may remain in the system after sample loading is finished Care must be taken to prevent this liquid reaching the pump 2 2 Evacuation of the sys...

Страница 7: ...n the sample is frozen a vacuum can be achieved by switching the pump to its roughing mode and opening valve V1 For a high vacuum switch the pump to turbo 2 2 3 Removing air from Vessel 3 Once the sys...

Страница 8: ...be read from the baratron gauge Tap B should be closed to prevent suck back of the liquid as the solid thaws The sample can be warmed gently to aid the thawing process and when complete close tap A 2...

Страница 9: ...t by cooling evacuation or both 2 4 1 Vessel 1 to sample cell The transfer of liquid from Vessel 1 to the sample cell is brought about by the difference in pressure between that in the Vessel and a va...

Страница 10: ...the sample cell When it is judged that sufficient liquid has been transferred to fill the sample cell close valve V5 At this point it must be remembered that the lower manifold contains liquid which m...

Страница 11: ...e evacuation procedure may be required The liquid may also be encouraged to leave the sample cell by using a small amount of gas Close valve V3 and open valve V9 to allow helium gas into this part of...

Страница 12: ...liquid may also be encouraged to leave the sample cell by using a small amount of gas Close valve V3 and open valve V10 to allow helium gas into the lower part of the system Close valve V10 and carefu...

Страница 13: ...he rig Muon spin resonance experiments were performed at 2 G and 20 G followed by reattached to the rig At this point the rig was open to the air and so had to be evacuated and pumped for 30 minutes T...

Страница 14: ...ond experiment all of the n hexane used in the first experiment was recovered into a sample bottle and dried using a small piece of clean sodium The liquid was carefully poured back into Vessel 1 and...

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