100ns Sweep window, at 760,350,000ps delay:
Tab 'Ramp': Advanced shows TR:0 0 150 , SP:0 0 200
20ns Sweep window, at 760,500,000ps delay:
Tab 'Ramp': Advanced shows TR:0 0 75 , SP:0 0 200
5ns Sweep window, at 760,713,000ps delay:
Tab 'Ramp': Advanced shows TR:0 0 0 , SP:0 0 0
200ns Sweep window,
Tab 'Ramp': Advanced shows TR:0 2 0 , SP:0 0 200
1us Sweep window,
Tab 'Ramp': Advanced shows TR:0 9 0 , SP:0 4 0
5us Sweep window,
Tab 'Ramp': Advanced shows TR:0 26 0 , SP:0 4 0
Update for all the stuff that happened last week and yesterday.
For the Students and their imaging:
Inlite Laser Update:
Gil got in early, and ran a Q3xQ1 runs with thick acrylic.
im trying the same runs, but with 3.5mm step size. First set with 4mm Teflon(550keV Stopping) then 6mm teflon(700keV stopping).
I ran simulations on the different quadrupoles configurations.On my personal laptop Jupyter. We physically test Quad1 with 2,1, then 3 magnets per pole, then Quad1 with 3 and Quad2 with 1 magnet. Look for the times started to know when each starts. as well as the image to know when the Quads are Flipped up or down.
we used the Teledyne_3 (Off Brem)
Q3xQ1: BG:295103, Strt:295104, End:295823
Q3xQ0: BG:294262, Strt:294263, End:295102
Q1xQ0: BG:293421, Strt:293422, End:294261
Q2xQ0: BG:292307, Strt:292308, End:293420
THÉODEN = Tapered Housing Extraction Of Diverging EmissioN
Found the Equation the relates the focal length to the a magnetic field strength and energy of the electron
When approximating for the thin Len ray equation, you miss a factor of 1/2, where you you would have caught it if you did Busch’s theorem. Which accounts for the rotation the electron will do, which then you take the average of the movement in both the xy-plane.(adding the 1/2)
f_Busch’s theorem = 2*f_thin lens
Yun Kai came to the lab. We got the short pulse and long pulse to meet at TCC. We use Frodo's green laser and another green diode laser to align the beams, plus send the light to Frodo's Basler and the Streak Camera. The short pulse is very sensitive, since the travel distance is so much longer.
We were able to get an image of the both pulses, on our cameras, by inserting a Microscope slide at TCC to reflect the short pulse.
Notes for warming up:
Notes for next time:
over the break oscillator was working but didn't mode lock when we got back. we walked the 2 cavity mirrors and the stepper motors to get a small mode lock. we ultimately Set the Stepper Motors to Default, Greased the slit motor threads. and did very small adjustment to the horiztonial knob of the M7 mirror. it became way more consistent now.
The slit motor travel is about 23mm or 87k counts.
the configuration for the MIT Users are 800nm at 40mJ after the Amp, with 0.8mm diameter beam, and 300ps pulses.
Damage threshold is Energy/ Area. and Power is Energy/PulseTime
Our laser rating for damage is 0.0795J/cm^2. per pulse