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Jim Sullivan.  Big Bang Theory  Dark Matter and Dark Energy  Detecting Dark Matter  Radiation and Pulse Shape Discrimination  SNOLAB  Summary.

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Presentation on theme: "Jim Sullivan.  Big Bang Theory  Dark Matter and Dark Energy  Detecting Dark Matter  Radiation and Pulse Shape Discrimination  SNOLAB  Summary."— Presentation transcript:

1 Jim Sullivan

2  Big Bang Theory  Dark Matter and Dark Energy  Detecting Dark Matter  Radiation and Pulse Shape Discrimination  SNOLAB  Summary

3  Saw Dark Matter by effect on galaxies and speed of stars  Even the arrangement of galaxies controlled by Dark Matter  But how can we measure it on Earth?

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6 V star F=m s V 2 /r F=G m g m s /r 2 r

7  May be type of sub-atomic particle – ◦ WIMPs (Weakly Interacting Massive Particles) ◦ Axion (small mass, no electric charge, weak interaction)  Current effort focused on WIMPs  Properties of WIMPs ◦ Weakly interacting –  Surrounded by it and don’t notice ◦ Massive –  Enough gravitational force to hold a galaxy together

8  Standard solid state radiation detectors – been tried, not successful yet, expensive and difficult to make large enough  Liquid argon detector ◦ Collision between WIMP and argon nucleus like billiard balls ◦ WIMP has lots of kinetic energy (earth moving through space) causes Ar recoil ◦ Enough energy to excite electrons in recoil ◦ Burst of light energy as atoms return to ground state, detected as photons

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10  Noble gas  M.P. 83.8 K (-189.4 o C)  B.P. 87.3 K (-185.8 o C)

11 Ar WIMP

12 Ar

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14  When atom returns to ground state, gives off photon  Use photomultiplier to detect photon

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16  Probability of WIMP hitting an Ar atom very small ◦ Weakly interacting  The more Ar atoms, the bigger the overall probability  The bigger the tank, the bigger the probability

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19  Don’t detect WIMP directly  WIMP excites argon atom  Atom gives off photon  Measure the photon  Do we detect anything else?  Yes, radiation  So…..

20  …Radiation and Pulse Shape Discrimination


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