#1930 baseline transfer Higaki A = 3.5, HigakiB = 5.5 V 
Increasing Higaki B to see if the 2nd peak reduces
#1931 HigakiB = 6.0 V 
MCP inserted to identify location of annihilation peaks
#1932 MCP in beamline 
The peak we are trying to reduce is certainly after the MCP (so likely the entrance to the Cusp trap electrodes)
#1933 HigakiB = 8.0 V 
This made matters worse, we suspect maybe it over focuses the pbars into the cusp
#1934 HigakiB = 7.0 V 
Seems the annihilation point has moved further upstream on the Cusp trap
Now we try below 5.0 V the inital conditions in #1930
#1935 HigakiB = 5.0 V 
#1936 HigakiB = 4.0 V 
#1937 HigakiB = 3.0V 
Seems like Higaki B isn't improving
revert to HigakiB = 5.5 inc Higaki A from 3.5 to 4.5V
#1938 HigakiA = 4.5 V 
#1939 Higaki A = 4.5 V, Higaki B = 4.5 V
#1940 Higaki A = 4.5, Higaki B = 6.5 V 
#1941 Higaki A = 4.5, Higaki B = 7.5 V 
#1942 Higaki A = 5.5, Higaki B = 6.5 V 
#1943 Higaki A = 5.5 V, Higaki B = 7.5 V 
#1944 Higaki A = 5.5 V, Higaki B = 5.5 V 
Looks like we now hit all of the chambers as the beam passes from MUSASHI to the Cusp ?
#1945 Higaki A = 2.5, Higaki B = 5.5 V 
#1946 Higaki A = 2.5 V, Higaki B 4.5 V 
Suspicion now that the peak we can't ever seem to change is the microwave blocking grid...
--Suspicious it is a large ammount of annihilation for a 98% transmission grid (well it's not Dan san it's 79%)...
#1947 Higaki A = 2.5 V, Higaki B = 6.5 V 
#1948 Higaki A = 2.5, Higaki B = 7.5 V 
#1949 Higaki A 3.5, Higaki B 5.5. Float potential (pbar energy) 50eV 
Dan san wanted to see what happened when you change the transfer energy...
Transfer to cusp GV
#1950 Higaki A 3.5, Higaki B = 5.5 V GV closed 
Set float to 150V --> higher energy transfer (some would say too high for the Cusp amplifiers but I guess it's just a quick test)
#1951 Higaki A = 3.5V, Higaki B = 5.5 V 
Open Cusp entrance GV with 150 eV transfer energy (which someone did say was too high energy for the cusp amps)
#1952 Higaki A = 3.5, Higaki B = 5.5 
Trying to identify the features 
Higher energy is easier...
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