Discovery 2020
Yuta Michimura
Department of Physics, University of Tokyo
April 21, 2020 Ando Lab Midterm Seminar
Discovery 2020 Yuta Michimura Department of Physics, University of - - PowerPoint PPT Presentation
Ando Lab Midterm Seminar April 21, 2020 Discovery 2020 Yuta Michimura Department of Physics, University of Tokyo Contents Looking back on the year 2019 Working from home My plans and expectations for the year 2020 Hot topics
Yuta Michimura
Department of Physics, University of Tokyo
April 21, 2020 Ando Lab Midterm Seminar
Space Interferometer Laboratory Voyaging towards Innovative Applications
Contents
2
(c)Philip FONG / AFPReview: My Plans JFY2019
3 Only upto ~0.97 Mpc Mostly not done Done for some tables KAGRA+ paper not done Work in progress (Paper with Somiya-san published) SILVIA Cavity constructed New collaboration started (PnC, LMA)
Review: My Expectations JFY2019
4 Successful implementation Paper by Enomoto-kun Not achieved Partially done DONE at below 100 Hz Achieved good sensitivity but not started Cryostat constructed PASSED From this year? DONE
Effort Report for 2019
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Effort Report for 2019
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* Number of days spent was counted for each topic based on my personal record. If n topics on the same day, 1/n was allocated for each topic. For 2018
45.0% 19.9% 4.6% 0.0% 4.7% 2.3% 15.6% 8.0% without VirgoEffort Report for 2020 (so far)
7
brain and PC (which is not ideal for experimentalists, though)
Working from Home
8
Sleep Sleep Eat Eat Eat Eat Eat Work Work Commute News Shop Chat
(may be just a coincidence)
Email Traffic over the Month
9
7都府県 緊急事態宣言 https://emailanalytics.com/ Started to work from home Test emails to check granite
mirror started as anticipated
tragedic issues: birefringence and frosting)
including lectures at TianQin Research Center and Durham University, and met new people
Parity article on KAGRA
Summary and News from JFY2019
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Productivity for the Past 10 Years
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As of April 2020 B4->M1 PhD ThesisNumber of People in Ando Group
12
Grants for JFY2020
13 Lorentz violation
Optical levitation
Quantum
Axion
※間接経費含む
very important in coming years
……
Balance between Topics
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to TRX and TRY of KAGRA
with KAGRA data
My Plans JFY2020
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rotation
curvature from coating stress)
My Expectations JFY2020
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→ postponed to June 2021
Schedules in JFY2020
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towards Innovative Applications
Hot Topics
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sensitive to various physics other than gravitational waves
Laser Interferometry
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Laser
Length change δL/L Gravitational waves Axion Lorentz violation Speed of light change δc/c Fringe change ∝δL/L, δc/c anisotropy
Quantization
Mirror displacement Non-standard forces
Dark matter Dark energy
polarization dependence B-L bosons Cosmic expansion, inflation Alternative polarization modes wave function collapse quantization of spacetime Boson cloud around BHs extra dimensionswe know they played an important role in forming our Universe, but we don’t know what they are at all
Dark Matter
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Past Searches: WIMPs
22
PBHs (upto 100 Msun = 1e59 GeV)
Park (2007) https://cerncourier.com/a/defeating-the-background- in-the-search-for-dark-matter/A New Era
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dark matter)
(DANCE)
Laser Interferometric Search
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DANCE
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phase velocity between left-handed and right- handed circular polarizations
as resonant frequency difference in an bow-tie cavity
coupling constant axion field axion mass
DANCE Act-1
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∝ma ∝ma 1/4 ∝ma 5/4 Tcoh>Tobs cavity pole ∝ma 1/2 scan ∝ma 1/2 scan ∝ma 1 ∝ma 5/4experiments like GW detectors
DANCE Act-2
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γ-ray from SN1987A CAST
Axion-photon coupling
DANCE Act-2 (two cavities)
X-ray from M87
KAGRA (3 km)
Advanced LIGO (4 km)
DM Axion Search with GWDs
detectors
modulation in polarization angle of linear polarization
light in a cavity are the same
along with GWs
28
left-handed is faster right-handed is faster p-pol
Modulation at frequency
Laser FI p-pol s-pol (Axion signal) p-pol (GW signal)
symmetry → It is natural to think that some gauge boson is coupled
through leptogenesis
B-L Gauge Boson
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Baryon Lepton
浜口幸一 (2017)GW detectors and mg-scale optomechanical experiments
B-L ratio (~neutron ratio), different resonant frequency, or mirrors are apart, amplitude or phase of force acting on mirrors are different and DM signal remains
Gauge Boson Search
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sapphire mirrors
Search with KAGRA and mg Mirror
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When DM direction is optimal 1 year observation with designed sensitivity for KAGRA and aLIGO Sensitivity in PRL 122, 071101 (2019) is used for 7-mg pendulum
KAGRA PRC
KAGRA DARM
Advanced LIGO EP tests 7-mg pendulum with fixed mirror
bring light to KAGRA
bKAGRA to dKAGRA
32
Sensitive axion search with OFI rejected beam B-L gauge boson search with POP beam Add polarization
and TRY to search for axion with lower sensitivity
JGW-P2011614
Fine-Structure Constant
mirror thickness change
position change by DARM
33
PRR 1, 033187 (2019)
(Primakoff effect)
Light Shining through Wall (LSW)
34
production γ→a reconversion a→γ
power build up magnetic field cavity length
Proposal to Improve the Sensitivity
35
FPAS-100 B=10 T, L=100 m, Finesse=1e5, Pin=7.5 W ALPS-IIc B=5 T, L=100 m, Finesse=1.2e5, Pin= 30 W
3 mm dia. t 0.1 mm, RoC= 30 mm, R>99.95 %
Long History
37
Levitation Mirrors We Want
finesse is OK
38 For SQL Prototype For suspended experiment Mass 0.2 mg ~1.6 mg ~ 7 mg Size (mm) φ 0.7 mm t 0.23 mm φ 3 mm t 0.1 mm φ 3 mm t 0.5 mm RoC 30 mm convex 30±10 mm convex (measured: 15.9±0.5 mm) 100 mm concave (previously flat
Reflectivity 97 % (finesse 100) >99.95 % (measured: >99.5%) 99.99% Comment
Optics Express 25, 13799 (2017)
Only one out of 8 without big cracks Succeeded
allowed from diffraction loss
Mirror Mass vs Reflectivity
39 Calculation by T. Kawasaki, modified by YM
(Mirror thickness 0.1 mm, fused silica assumed to calculate radius. Critical coupling)97%, 0.2 mg (for SQL)
If critical couple, no detuning 9.8 m/s2 Mirror power transmission (R=1-T) Intra-cavity power
99.95%, 1.6 mg (for levitation demonstration)
Beam radius should be smaller than 0.6 mm Beam radius has to be smaller than dotted lines (2*Taperture < T coat/10)Mirrors to Characterize in 2020
40
(Nagano method; see JPS2017s talk)
Characterization Method
41
Absorption
42
for calculating surface area
will be higher by x~2 if upper cavity is also considered Temperature for disk shape saturates when radius >> thickness since m, Pcirc and A will be proportional to radius2
Surface area Mirror temperature Environment temperature Emissivity(~0.99) Stefan-Boltzmann constant Absorption
also have to be considered
etc… should be considered with simulations
(fused silica melting point is ~2000 K)
(if mirror heating increases cavity length, single optical spring can stabilize the cavity length)
More on Absorption
43
Nanosphere is Hot
44
Even though absorption is low, high temperatures (2,000 K) can be reached because of poor heat transfer to the surrounding gas at low pressures.
and monolithic optics
noise floor at stationary and rotation achieved by Takeda-kun
Even Longer History
46
Apparatus Comparison
47turntable laser semi- monolithic
vacuum enclosure data logger AC power turntable laser non- monolithic
vacuum enclosure data logger AC power rotary connector
Old Model
New Model
PC PC wireless
stationary
Latest Sensitivity
48
When rotating (old) When rotating (new) Stationary (old) Stationary (new) Polarization? Intensity? Could be solved with fiber fusion splicing
toward the observation (may be its better to just start now?)
hunting
space (see seminar slides)
Prospects in 2020
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http://qsfp.physics.ox.ac.uk/SILVIA
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Sensitivity
52
SILVIA
TOBA
B-DECIGO LISA TianQin B-DECIGO LISA
aLIGO Cosmic Explorer Einstein Telescope KAGRA
Control Scheme
53
Laser
GW signal frequency servo length servo drag-free servocontrols taken into account
and here), but actual demonstration in table-top experiments and time-domain simulations are very important
noise, focus on scheme
Interesting Topics for SILVIA
54
(cavity characterization, noise spectrum…)
(similar to continuous wave search; we are taking KAGRA PRCL and MICH data now!)
(alignment, scattered light, fiber splicing…)
Job Advertisement
55 * Red ones can be done from home
motivate yourself
Summary
56