split magnet and optics program jack toth scott bole scott gundlach jim o’reilly magnet science...

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Split Magnet and Optics Progr Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR Scientist

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Page 1: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

Split Magnet and Optics Program

JackToth

ScottBole

ScottGundlach

JimO’Reilly

Magnet Science and Technology

SteveMcGill

DmitrySmirnov

DC Fields

FTIRScientist

Page 2: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR
Page 3: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR
Page 4: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

Wonderfully Complex Magnet

“Wheel”

Split Florida-Helix Technology

Page 5: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR
Page 6: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

SpeakersSteve McGill

Janice Musfeldt Junichiro KonoSteven Cundiff

Gregory ScholesAron Pinczuk

Girsh BlumbergKresimir Rupnik

Matt SfeirDmitry Smirnov

Page 7: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

New Experimental Capabilities• Raman Spectroscopy

o Doing with fibers, but limited in sensitivity and geometrieso Split Helix gives large angleso Carbon and semiconductor based nanostructures (graphene, quantum wells,…), phase

transitions, HTS, quantum spin systems…• THz-Time Domain Spectroscopy

o generate low power broadband short pulseso uses FFT to recover both amplitude and phase information from interaction with sampleo ac conductivity of superconductors in high fields, cyclotron resonances…

• Optical 2D Fourier Transform Spectroscopy and 4-wave Mixingo sensitive interferometery that combines 3 or more beams of lighto cutting edge techniques, impossible without the Split-Helixo probes excitonic systems and their dynamics

• Improving existing methods:o Photoluminescenceo Infrared magneto optics (FTIR…)o EPR/ESR

Split magnet enables the ability to do “micro- spectroscopy”, imaging, etc. with many techniques

X-ray opportunities

FEL opportunities

Page 8: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

Shopping List

• U-shaped non-magnetic optical table around magnet (150 k$)• Optical windows, custom vacuum hardware… (200 k$)• Dewar/cryosystem mounted to optical table (350 k$)• Vibration isolation between dewar and magnet (100 k$)• Narrow band Krypton laser for Raman Spectroscopy (100 k$)• Time correlated photon counter (100 k$)• Micropositioners & rotators, high B/low T (400 k$)• Optics, detectors, etc (400 k$)• New Bruker FTIR spectrometer with microscope (250 k$)• New, small footprint one-box amplifier ultrafast laser system (1 M$)• Custom made ultra low frequency Raman Scattering spectrometer

(including custom microscope) (1 M$)

Page 9: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

Personnel

• Technician – being hired• 3 Postdocs – optics, FTIR, micro-Raman/optics• Grad Students• Senior Faculty Member?

Page 10: Split Magnet and Optics Program Jack Toth Scott Bole Scott Gundlach Jim O’Reilly Magnet Science and Technology Steve McGill Dmitry Smirnov DC Fields FTIR

Installation into Cell 5Open wall to Optics Cell (3), extend ceiling, 100 k$