31
SLIDE 1 Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus Part of Disk Receding end of jet SW Fibre systems for cosmology

Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

  • Upload
    others

  • View
    0

  • Download
    0

Embed Size (px)

Citation preview

Page 1: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

SLIDE 1

Jeremy Allington-Smith and Graham Murray

Centre for Advanced Instrumentation University of Durham

Approaching end of jet

NE

Nucleus

Part of Disk

Receding end of jet SW

Fibre systems for cosmology

Page 2: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Content

• Some critical issues for DESpec

• Some technology examples

• A radical approach to make DESpec unique

Note: due to MOA with BigBOSS I can’t give details of specific technologies developed with LNBL

Page 3: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

SLIDE 3

Rochester Building NetPark Research Institute Astronomy spectroscopy and Adaptive Optics, Nuclear fusion, Biophysics, Earth observation

Latest spectroscopy news: Instruments: KMOS, SALT-HRS, JWST-NIRSpec IFU R&D: Diverse Field Spectroscopy, Astrophotonics,

3D-Heliospectropolarimetry

Page 4: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

BigBOSS and DESpec

BigBOSS DESpec

FOV (linear) 3.0 2.2 deg

N Targets 5000 4000

Subfield 180 110 arcmin

Pitch 12 6.8 mm

Fibre input focal ratio

F/4.5 F/3

Wavelength range

340-1060 600-1000 nm

Resolving power

3000-4800 1900-3300

Page 5: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

BigBOSS fibre system

Fiber Ferrules at Actuator

Fiber Support& Distribution

Cable Junction BoxConnectors

Cross Spider CableMain Cable(s) Cable Rotation Guide

Cable Suspension

Slit Assemblies

Multi Connector

Cable Rotation Guide

Fiber & Support System

Cable Junction BoxConnectors

2Tuesday, July 26, 2011

Slide by BigBOSS (LNBL)

Page 6: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

The BigBOSS philosophy

• Scrupulous attention to all sources of uncertaintiy

– Throughput • “Soup to nuts” models

– Variation of throughput • fibre-to-fibre

• Position-to-position

• Time-to-time

• Dynamic error budgets (systems engineering) • Top-down reallocation of error sources

• Top-down must match Bottom-up

• Minimise cost/fibre

Page 7: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Some generic issues for fibre system

Number of actuators > speed of survey

Pitch & filling factor > speed of survey/clustering

Fibre throughput & AR coatings > speed of survey, λ λ, cable length

Positional accuracy/repeatability > throughput & survey strategy

Alignment to telescope exit pupil > FRD & Numerical Aperture

Alignment to spectrograph pupil > slit design, Lenslets?

Repeated fibre flexure, torsion > breakage, wind-up, light loss

Environmental changes > modal noise -> SNR limit

Mechanical flexure of focal plane > holey structure, weak?

Fibre replacement strategy > how and when?

Connector strategy > how many, where?

Page 8: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Etendue violation

Non-conserve of Etendue: Focal Ratio Degradation

– Intrinsic effect due to modal diffusion from defects • Caused by manufacture and stress during operation

• Critically dependent on fibre termination

• Macrobending (if ROC < 1000 x fibre radius)

– Extrinisic effects due to misalignment with fibre axis • Intentional (tilting spines)

• Unintentional (errors in construction)

– Extrinsic effect due to scattered light (e.g. D. Haynes et al)

• Requires good polishing and/or index-matched immersion to smooth optic

Page 9: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Field-dependent FRD

Limiting Numerical Aperture Light loss into

cladding

Alignment error

Polishing error

Intrinsic FRD

Spectrograph stop

Page 10: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Telescope exit pupil match

Best focal plane

Defocus and tilt error due to: - Non-telecentricity - Field-selector tilt

Focal surface

Subfield

TS Field- selector

Telescope exit pupil

Generally not telecentric

Page 11: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Pupil configuration at slit `To place pupil on spectrograph disperser requires a field lens close to the input spectrograph focal plane.

This creates a virtual input pupil to which fibres must be aligned.

(For a beam-fed spectrograph, the virtual spectrograph pupil would be coincident with the telescope exit pupil.)

Virtual Entrance pupil

Real spectrograph

pupil

Collimator Field lens (near focus)

Disperser

Slit

Acceptance Beam of fibre

Page 12: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

SLIDE 14

Modal noise

Limit to fibre spectroscopy SNR

• interference between partly-coherent

waveguide modes

• Speckle statistics altered by limiting

apertures (e.g. spectrograph stop)

• may affect line position and shape

• Affects higher spectral resolution?

Traditional solutions: agitation

• Feasibility for a multi-fibre system?

Modal noise prediction in fibre-spectroscopy I: Visibility and the coherent model, U. Lemke, J. Corbett, J. Allington-Smith, G. Murray. MNRAS 404, 1349.

Without agitation

With agitation

1000

5000

SNR

Integration time

Page 13: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Limiting Numerical Aperture

Caution near LNA: Need special fibre to avoid light loss

Near LNA, sensitive to misalignments and FRD (softened cutoff)

Allington-Smith et al. SPIE 2012

Page 14: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

SLIDE 16

Connectors? Pro

• Easier to integrate fibre system with telescope

• Routing thousands of fibres from pickoff to slit may be otherwise

impossible

• Easier/possible to replace damaged fibres

• Easier to share work between fabricators/collaborators

Con

• Throughput loss

• Variable insertion loss

Note

• Throughput for FMOS fibre system alone >80% (Kimura et al. 2010)

• Make/break connectors once-only (or once/year)?

• New technology using GRIN lenses has been prototyped

• Commercial options under investigation

Page 15: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Nida de Ratos

Fibres routed Via spider

Multifibre connectors Slide by BigBOSS

(LNBL)

Page 16: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Technology adapted from FMOS

• CfAI developed the fibre system: (Cable, connectors, strain relief, slit units)

• Fibres terminated at connector or focal surface

• Routed to through telescope structure

• Protected from stress by sophisticated yet robust cable and strain relief units

• Measured on-telescope throughput of the fibre system >80% (Kimura et al. 2010)

Page 17: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

FMOS

Page 18: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Fibres

Ceramic ferrule

Fibre core + cladding

Fibre buffer For protection

Adhesive layer Fixes fibre in ferrule

Sleeve for protection

~1mm

Fibres can be A/R coated

Page 19: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Fibre cable

Page 20: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Strain relief

Page 21: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

SLIDE 23

Slit units

Fibres immersed to glass meniscus with A/R coating

Page 22: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Lenses

Collimator barrel

with fibre and

ferrule

Ferrule

Fold prism and back illumination LED

Fibre connectors

Built-in back-illumination Upgradable to multiband

Page 23: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Vigorous underpinning R&D

Page 24: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Fibres are not the only fruit

Page 25: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

DEXMOS: Higher SNR with 10,000 slits

Better background-subtraction and calibration, spatial information

-> BAO: [OII[-emitters 4000 targets/deg2 for z < 1.5 => 20million redshifts in 200 nights*

-> Galaxy evolution: kpc-Mpc scale dynamical information for galaxies and groups

• 10 modular spectrographs (120 x 120 x 720mm3)

– Instantaneous field: 2.5 sq.deq with 1 slit mask

– Full corrector field in 1 passband in 2 visits

– Mix and match bandpass and field coverage

• 3 bands via exchange of VPH-grism & adjacent optics

– 560-750nm R=1500

– 750-900nm R=3000

– 840-870nm R=5000

• Hardware costs $4M

* Tom Shanks

Page 26: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

2.4 deg field (50% vignetting)

10 spectrographs 34’ x 26’ -> 2.5 deg2.

Gap size = half of field width so 3 images (moving by gaps size each time) give uniform transmission with each source observed twice.

Tiling the sky

50% of field in one passband simultaneously

Page 27: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

AC114 Mask

Page 28: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Preliminary DEXMOS spectrograph design using field scale and F-ratio of corrector and 720 mm between focal planes. Image quality (50%EED)

already better than slit width on average.

Cheap unit spectrographs Interchangeable disperser and close optics

Shanks & Content, SPIE 7014: 701475 (2008) [arXiv:0808.2367]

Page 29: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Mask & disperser exchangers

Designs for VISTA implentation

One mask/field Set of 10 dispersers/field

Page 30: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Concluding remarks

• Do BigBOSS and DESpec need to compete on hardware?

– Can you (time-)share in knowledge and/or hardware?

• Otherwise can DESpec do something unique and/or complementary?

– E.g. DEXMOS

Page 31: Fibre systems for cosmology - KICP Workshops · Jeremy Allington-Smith and Graham Murray Centre for Advanced Instrumentation University of Durham Approaching end of jet NE Nucleus

Fin