Kennedy Thorndike on a small satellite in low earth orbit

Similar documents
Pound-Drever-Hall Locking of a Chip External Cavity Laser to a High-Finesse Cavity Using Vescent Photonics Lasers & Locking Electronics

First step in the industry-based development of an ultra-stable optical cavity for space applications

A Low-Noise 1542nm Laser Stabilized to an

Frequency Stabilized Lasers for LIDAR 6/29/2016 Mark Notcutt and SLS Team Stable Laser Systems Boulder CO

1. INTRODUCTION 2. LASER ABSTRACT

레이저의주파수안정화방법및그응용 박상언 ( 한국표준과학연구원, 길이시간센터 )

Stability of a Fiber-Fed Heterodyne Interferometer

Interferometers for stability measurements

Low Vibration, Low Thermal Fluctuation System for Pulse Tube and Gifford- McMahon Cryocoolers

The AEI 10 m Prototype. June Sina Köhlenbeck for the 10m Prototype Team

LISA and SMART2 Optical Work in Europe

Testbed for prototypes of the LISA point-ahead angle mechanism

Installation and Characterization of the Advanced LIGO 200 Watt PSL

The VIRGO detection system

Highly Reliable 40-mW 25-GHz 20-ch Thermally Tunable DFB Laser Module, Integrated with Wavelength Monitor

A gravitational wave is a differential strain in spacetime. Equivalently, it is a differential tidal force that can be sensed by multiple test masses.

DESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE

R. J. Jones College of Optical Sciences OPTI 511L Fall 2017

Autotracker III. Applications...

SA210-Series Scanning Fabry Perot Interferometer

Next Generation Space Atomic Clock Space Communications and Navigation (SCaN) Technology

Wavelength Control and Locking with Sub-MHz Precision

Continuous-Wave (CW) Single-Frequency IR Laser. NPRO 125/126 Series

Angular Drift of CrystalTech (1064nm, 80MHz) AOMs due to Thermal Transients. Alex Piggott

Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series

First results of a high performance optically-pumped cesium beam clock

Lasers à fibres ns et ps de forte puissance. Francois SALIN EOLITE systems

A Narrow-Band Tunable Diode Laser System with Grating Feedback

Kit for building your own THz Time-Domain Spectrometer

Optical cesium beam clock for eprtc telecom applications

PULSE PIC- PULSE PICKING

Fast Widely-Tunable CW Single Frequency 2-micron Laser

Diode Laser Control Electronics. Diode Laser Locking and Linewidth Narrowing. Rudolf Neuhaus, Ph.D. TOPTICA Photonics AG

HIGH STABILITY LASER FOR INTERFEROMETRIC EARTH GRAVITY MEASUREMENTS

Laser stabilization and frequency modulation for trapped-ion experiments

Powerful Single-Frequency Laser System based on a Cu-laser pumped Dye Laser

Thulium-Doped Fiber Amplifier Development for Power Scaling the 2 Micron Coherent Laser Absorption Instrument for ASCENDS

Single-frequency operation of a Cr:YAG laser from nm

visibility values: 1) V1=0.5 2) V2=0.9 3) V3=0.99 b) In the three cases considered, what are the values of FSR (Free Spectral Range) and

Performance of the Prototype NLC RF Phase and Timing Distribution System *

UNMATCHED OUTPUT POWER AND TUNING RANGE

Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics

Extending the Offset Frequency Range of the D2-135 Offset Phase Lock Servo by Indirect Locking

This is a brief report of the measurements I have done in these 2 months.

Difrotec Product & Services. Ultra high accuracy interferometry & custom optical solutions

A transportable optical frequency comb based on a mode-locked fibre laser

R. J. Jones Optical Sciences OPTI 511L Fall 2017

Femtosecond Synchronization of Laser Systems for the LCLS

ABSTRACT 1 CEBAF UPGRADE CAVITY/CRYOMODULE

Designing for Femtosecond Pulses

Design and Manufacture of 8.4 m Primary Mirror Segments and Supports for the GMT

Assembly and Experimental Characterization of Fiber Collimators for Low Loss Coupling

Jaringan Komputer. Outline. The Physical Layer

VELA PHOTOINJECTOR LASER. E.W. Snedden, Lasers and Diagnostics Group

Satellite-based tests of Special and General Relativity

A novel tunable diode laser using volume holographic gratings

Eye safe solid state lasers for remote sensing and coherent laser radar

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT

taccor Optional features Overview Turn-key GHz femtosecond laser

Biomedical Research 2017; Special Issue: ISSN X

Low Noise, High Power DFB Laser Part #LN Pxx

and Tricks for Experimentalists: Laser Stabilization

Narrow line diode laser stacks for DPAL pumping

LIGO Photodiode Development and Optical Platform for LIGO Photodetectors Testing

Status Report on Time and Frequency Activities at National Physical Laboratory India

Capacitive sensors capancdt

Power scaling of picosecond thin disc laser for LPP and FEL EUV sources

Optical phase-coherent link between an optical atomic clock. and 1550 nm mode-locked lasers

A Penning Trap for Precision Spectroscopy of Highly Charged Ions at HITRAP. Jörg Krämer University of Mainz

Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL)

HIGH PRECISION OPERATION OF FIBER BRAGG GRATING SENSOR WITH INTENSITY-MODULATED LIGHT SOURCE

Lenses. Optional Reading Stargazer: the life and times of the TELESCOPE, Fred Watson (Da Capo 2004).

Orbit Stability Challenges for Storage Rings. Glenn Decker Advanced Photon Source Beam Diagnostics March 8, 2012

Actively Stabilized Scanning Single-Frequency. Ti:Sa /Dye Ring Laser External Doubling Ring Ti:Sa /Dye Standing Wave Laser

Faraday Rotators and Isolators

Zeeman Shifted Modulation Transfer Spectroscopy in Atomic Cesium

TechNote. T001 // Precise non-contact displacement sensors. Introduction

880 Quantum Electronics Optional Lab Construct A Pulsed Dye Laser

CubeSat-Scale Hyperspectral Imager for Middle Atmosphere Investigations

FPPO 1000 Fiber Laser Pumped Optical Parametric Oscillator: FPPO 1000 Product Manual

arxiv: v1 [physics.optics] 19 May 2016

MOI has two main product lines for its component business: 1. Tunable filters (FFP-TF, FFP-TF2, FFP-SI) 2. Fixed filters (FFP-I, picowave)

Arm Cavity Finesse for Advanced LIGO

UCI ZEEMAN EFFECT. Observe the fine structure lines of mercury and the Zeeman splitting of one or more of these lines as a function of magnetic field.

S.No Description/Specifications Qty 01. Post office box Trainer.

Fabrication of 6.5 m f/1.25 Mirrors for the MMT and Magellan Telescopes

confocaldt 2451/2471 Controller

E X P E R I M E N T 12

Design of a Free Space Optical Communication Module for Small Satellites

queensgate a brand of Elektron Technology

Development of scalable laser technology for EUVL applications

Differential Optical Shadow Sensor CubeSat Mission

Optical Isolator Tutorial (Page 1 of 2) νlh, where ν, L, and H are as defined below. ν: the Verdet Constant, a property of the

Advanced Virgo commissioning challenges. Julia Casanueva on behalf of the Virgo collaboration

The Lightwave Model 142 CW Visible Ring Laser, Beam Splitter, Model ATM- 80A1 Acousto-Optic Modulator, and Fiber Optic Cable Coupler Optics Project

Technical Report Synopsis: Chapter 4: Mounting Individual Lenses Opto-Mechanical System Design Paul R. Yoder, Jr.

Optical Microscope. Active anti-vibration table. Mechanical Head. Computer and Software. Acoustic/Electrical Shield Enclosure

3550 Aberdeen Ave SE, Kirtland AFB, NM 87117, USA ABSTRACT 1. INTRODUCTION

Nd: YAG Laser Energy Levels 4 level laser Optical transitions from Ground to many upper levels Strong absorber in the yellow range None radiative to

Waves & Oscillations

Transcription:

Kennedy Thorndike on a small satellite in low earth orbit Length Standard Development Shally Saraf for the JCOE Team Nice, 2013 1

STAR conceptual diagram 2

ministar conceptual diagram CUT 3

Optical cavity design at 10-15 stability Procure and shape material with minimal creep and ultralow expansion like ULE glass Coeff. of thermal exp. < 10ppb/K Develop supermirrors to obtain Finesse > 10 5 for high S/N R>99.9995% Operate the cavities close to the CTE zero-crossing point Active thermal control ULE backing rings + TEC s + cooling + servos Develop multi-layer sub microkelvin thermal enclosures Each layer attenuates thermal perturbations by >20X Develop fiber technologies to efficiently couple laser light into the cavity using an optical fiber Grin lenses + pointing control + fiber phase compensation (?) Develop servos for locking cavity to Iodine-stabilized laser FPGA control and science signal extraction 4

optical cavity in thermal enclosure Cavity 500g Enclosure 8750g 5

optical cavity material Key optical cavity parameters: L/L < 10-17 at orbit and harmonics with 2 years of data Derived requirements: Expansion coefficient: < 10-9 per K Operating temperature: within 1 mk of expansion null (~ 16-19 C nom) External strain attenuation: > 10 12 Stiffness: L/L < 10-9 per g, 3-axis Implied spacer: ULE glass Mirrors: Fused silica with ULE backing rings 6

thermal enclosure Main Requirements: Thermal stability Stress attenuation Launch and space compatible Thermal performance: Cavity L/L < 10-17 (2 yr data) at orbital period and harmonics Derived requirements (2 yr average): Thermal stability of 10-8 K at orbit Thermal gradient ~ 10-9 K/cm at orbit Maintain cavities temperature to 1 mk 7

thermal shield attenuation factors COMSOL MODEL 8

thermal modeling of 6-layer enclosure Multi-stage thermal filtering can give excellent control even for an equatorial orbit. ministar would need less layers for similar control. 9

deflection of cavities with acceleration worst case lab accelerations ~ 10-3 ms -2 at 30 Hz vertically Horizontal deflection per ms -2 4 nm 0.8 nm/div -4 nm a L top Vertical deflection per ms -2 21 nm a L botto m Short cavity ~ 200 khz/ms -2 0.5 nm/div 25 nm Support near geometrical center for CMRR Vertical orientation for symmetry DL cavity ~ pm 10

frequency/acceleration sensitivity 10 MHz/ ms -2 a = 0.11 * L 1 2200 khz/ms -2 0.1 150 khz/ms -2 a = 0.577* L a 0.01 5 6 7 8 9 1 2 3 4 5 6 7 8 9 10 2 3 4 5 6 7 8 9 100 2 L 11

vibration insensitive optical cavities STRAIN DISTRIBUTION Zero relative displacement at the ends of the optics axis Static Load applied at the points marked on the perimeter 12

strain attenuation model - FEA Estimated strain attenuation: > 10 3 per can Extrapolating to entire enclosure: > 10 15 Exceeds requirement by x1000 13

fundamental frequencies The first mode of the assembly was found to be 77 Hz First lateral mode: 77.6 Hz First axial mode: 93.9 Hz 14

possible mstar cavity designs (GRACE FO) 15

fiber coupling: ray tracing for fiber GRIN-lens system x1 x 1 4 3 2 1 d 1 z d 2 x x 2 2 1 0 1 cos cos 0 0 cos cos sin cos sin cos cos cos 0 0 cos cos 1 0 1 16

fiber-lens assembly at 1550nm 0.9mm 42mm 20mm Fiber Pigtail Grin Lens f = 1.9mm Regular Lens f = 12 mm Backup Tube Measured w 0 = 378.5 μm @ 20 mm after lens 2 (Could be adjusted to ~200 mm for longer working distance) Optimal w 0 = 375 μm for 10 cm cavity with flat & curved mirror (Rcc = 1 m) Total distance from fiber pigtail to second lens is ~42 mm 17

direct coupling into cavity Direct coupling arrangement Alignment adjustment through two sets of set screws Optical System is longer especially if transmitted light is collected. 18

right angle prism solution Coupling into cavity through right angle prism Alignment adjustment through two sets of set screws Optical System can be made compact reducing size of thermal enclosure. 19

basic fiber-coupled cavity layout 20

ministar optical diagram RF modulation obtained by frequency generation board RF demodulation executed digitally by FPGA board (with RF ADC channels) Digital VCO by onboard FPGA Laser PZT and Temp controlled by FPGA Science signal contained in the digital VCO error signal 21

optical cavity work at Stanford 1064nm ULE cavities with fused silica mirrors and ULE backing rings operating in a 2-layer thermal enclosure at10-9 torr. Currently tracking CTE null Beat note between cavity and I 2 @ 10-12 stability 22

iodine MTS setup at Stanford 1110 line R(56)32-0 is best Lock laser to the a 10 HFS Sub-doppler detection Modulation Transfer Spectroscopy (MTS) Natural Linewidth ~ 400KHz Broadened line < 1MHz Investigate narrower lines at ~508 nm 23

iodine setup at Stanford 24

mstar instrument concept in 3U CubeSat configuration Motherboard, CPU, Radio PDH, counter boards chassis Thermal & magnetic enclosure for optics Spherical optical cavity Thermal enclosures for cavity Electrical power system w/ batteries (30 W hr) AOM x2 Circulator Optical bench Cobolt 04 01 532nm laser Iodine cell (2cm long) 25

double conical optical cavity within UV-LED footprint 26

project schedule 27