Jessica Gifford | August 25, 2010 | Int-Reu.  Gravity Waves and Lisa  Torsion Pendulum  Old Electron Gun Measurements  New motor  Photocurrent measurements:

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Presentation transcript:

Jessica Gifford | August 25, 2010 | Int-Reu

 Gravity Waves and Lisa  Torsion Pendulum  Old Electron Gun Measurements  New motor  Photocurrent measurements: Data and Design  Autocollimator and Temperature 2

 Einstein’s General Relativity  Predicts gravity waves  More massive, more curvature, more gravity  The universe is mostly Minkowski space  Space Time Curvature is only as small effect 3 t0t0 t1t1 t2t2  Gravitational Radiation  Detection: Oscillations in space time.  As location of masses change with time so does the curvature

4 5 million km 50 million km Laser off of masses

 Pendulum is supported by a thin fiber and is allowed to hang freely  Pendulum reacts to the amount of charge on it from the electrodes  An electron gun is used to negatively charge the pendulum  UV LED is used to positively charge the pendulum  Plates are able to move  Changes in angle are measured using an autocollimator  Feed back loop is used to “catch” the pendulum and keep it on the detector 5 Solar rays can charge pendulum causing problems… Torsion pendulums correct for this:

 Electron source  Magnesium that is evaporated onto aluminum 6  Electron gun  Electrons are ejected from magnesium by the photo effect and negatively charge the pendulum

 Demonstration of charge control 7  Data  Intervals of 30seconds dictated by the time used to switch polarity of the plates  Polarity is switched to show that charges are measured from the pendulum  This is to show that the pendulum charge is measured not the electrodes and to show that it is independent of the polarity of the voltage that is applied to these feedback electrodes  Procedure  Pendulum is locked in feedback using a feedback loop  Also called “catching”  Use the electron gun to charge negatively  Use the UV LED to positively charge the pendulum  Issues  Temperature fluctuations  Timing Gun off and LED on

8 Time (s) Noise Runs at various positions  Noise Data  Want to see if there is distance dependence  Taken over night 8 separate days  Taken at 9 different distances ranging from 2mm-8mm in 1mm increments 2mm 3mm 4mm 5mm 6mm 7mm 8mm V+ + V-

 Installed new stepper motor 9  Built device to measure photo current of our UV LED  Criteria: Compatible with Pontech controller  Bipolar  Need ~5V : 4.2V  No more then 2A: 1.4A (we measured 2A)  Compact size around 4mm : 2mm  Materials  Magnesium Cathode  Aluminum cylinder and lid  Insulation  UV Led

10

Cathode Candidates ElementWork Function Caesium2.10 eV Rubidium2.16 eV Sodium2.28 eV Pottasium2.30 eV Calcium2.90 eV Lithium2.90 eV Magnesium3.66 eV 11 Magnesium Mesh Einzel Lens UV Led (330nm,3.8eV ) (244nm,5.1eV) Aluminum Plate Insulation

Used two different Led’s with no Einzel Lens  Current leakage  Noise regime  Signal drastically changes when you are in the room 12 Built battery system for the UV Led power  Fixes current leakage LM317

 Using a DAQ program: Integrated the power supply to be controlled by program 13 Time (fraction of day 236) Current (nA) Time (fraction of day 236)

 Took current measurements from -5V to 5V  Expect the current to rise at higher voltages and level off at more negative voltages  Do see a drop around -5V  More investigation is needed to see if this is photocurrent and for what ranges of voltages we see the change 14 Voltage (v) Current (nA) Voltage (v)  Photo Current Measurements with DAQ

 System of two lasers created by a diffraction grating  First laser is stationary and second one moves relative to it  Noise issues:  Sound  Mechanics  Thermal 15 Torque (pNm) Frequency ( mHz)

16  Built a system of two thermometers to measure thermal changes of our set up Output to DAQ

17  Temperature Data  First took raw temperature data  Data taken inside and outside the box  Peaks represent different noise components Temperature (C) Time (fraction of day 201)

 Take power spectral density measurements of the distance data for the LISA pendulum  Take new data with the motor  Vary the voltage between the Mg and Al of the electron gun and take photo current measurements to show that we are in fact measuring photocurrent and for what voltages  Test full design of electron gun with Einzel lens  Integrate the autocollimator and temperature programs so they can be correlated at the same times  Larger goal: Redesign autocollimator after temperature characterization 18

Thank you to: Stephan Schlamminger: Advisor -Charlie Hagedorn: Graduate Student -Jens Gundlach : Professor -David Hyde: Shop Manager - Ron Musgrave: Machine Shop Inst. -Gravity Group Members CENPA faculty and staff Special Thanks to : -Alejandro Garcia -Deep Gupta -Janine Nemerever -Linda Vilett For making this REU experience possible 19