1 martin elvis, astrophysics 2020, 14 november 2007 active x-ray optics for the next high resolution...

23
1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian Center for Astrophysics Cambridge, Massachusetts, USA

Upload: milton-joshua-bradley

Post on 13-Jan-2016

215 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

1

Martin Elvis, Astrophysics 2020, 14 November 2007

Active X-ray OpticsFor The Next High Resolution X-ray Observatory

Martin ElvisHarvard-Smithsonian Center for Astrophysics

Cambridge, Massachusetts, USA

Page 2: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

2

Martin Elvis, Astrophysics 2020, 14 November 2007

good enough for my thesis

1982 HEAO-11/100,000

2002 Chandra

45 Years of X-ray Astronomy:1 billion times more sensitive

2022 Gen-X

Detector Area, Exposure time

angular resolution

Good for 1 (one) Nobel Prize

1962 Sco X-11/10,000

1962 20071978

Page 3: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

3

Martin Elvis, Astrophysics 2020, 14 November 2007

The Chandra Revolution:Quantitative : 70 to 1400 Sources

ROSAT: ~10”The Star Formation Region in Orion

ROSAT: ~5”

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Chandra: ~0.5” [2.4 rad]

Page 4: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

4

Martin Elvis, Astrophysics 2020, 14 November 2007

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

The Chandra Revolution: Qualitatively new Features

ROSAT: ~5”

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Hubble: ~0.1”

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Chandra: ~0.5”

The Antennae Colliding Galaxies System

Page 5: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

5

Martin Elvis, Astrophysics 2020, 14 November 2007

A High Resolution X-ray Successor to Chandra

Obviously desirable Obviously infeasible? Have to define what is needed Derive Technology

requirements Pursue promising technologies

Page 6: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

6

Martin Elvis, Astrophysics 2020, 14 November 2007

The First Galaxies and Black Holes:X-rays at z~10-20

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Faint: 1st BH fluxes: ~10-3 of Deepest Chandra surveys

Area, Aeff ~ 100 m2

Angular resolution HEW ~ 0.1”, 0.5rad Reduce background Discriminate from foreground z=3 galaxies

Energy range0.1-10 keV spectra kT~10keV / (1+z) ~1 keV

Defines next generation high resolution large X-ray Observatory:

Generation-X

Z=10, Age = 480 Myr, 3.5%)

Page 7: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

7

Martin Elvis, Astrophysics 2020, 14 November 2007

A High Resolution X-ray Successor to Chandra: Issues

No current plans for a Chandra-class - sub-arcsec - mission - world-wide

No space agency developing high resolution X-ray mirrors

Reason: Cannot make a bigger Chandra mirrors are heavy

1.5 cm thick glass cylinders Can’t use integral shells

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 8: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

8

Martin Elvis, Astrophysics 2020, 14 November 2007

A High Resolution Successor to Chandra:New Mirror Technology

Mass/unit area (kg cm-2)

1.00.0 0.5

1

10

100

HE

W (

arcs

ec)

Chandra

Citterio et al.199x [Brera]

Con-X

Page 9: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

9

Martin Elvis, Astrophysics 2020, 14 November 2007

Generation-X Vision Mission Study

Gen-X selected as NASA Vision Mission study in 2003

0.1” FWHM 100 m2 @ 1 keV Nominal Launch date ~ 2020 Mission concept studies

JPL ‘Team-X’ : formation flying GSFC ‘IMDC’: single spacecraft

No Show Stoppers Mirrors are the greatest challenge

Generation-X Vision Mission Study Report March 9, 2006

Prepared for

National Aeronautics and Space Administration

(NASA) Headquarters

On-orbit adjustment of figure?

Page 10: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

10

Martin Elvis, Astrophysics 2020, 14 November 2007

Active X-ray Optics Solution:

Piezoelectric Bi-morph (PBM)

• Working at Synchrotrons

• news to astronomers

• 10 year program by Signorato et al.

• Operational

• 16-, 32- element

• ~1 m long optics

• 2 cm sized actuators

• Kirkpatrick-Baez configuration

16-element PBM

Signorato et al.,2004, SPIE

Page 11: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

11

Martin Elvis, Astrophysics 2020, 14 November 2007

Active X-ray Optics:

figure improvement

• Need factor ~100 correction:• ~400 nm errors to ~4 nm

• Finite element analysis shows feasibility of control… in principle!

log

Po

we

r (m

m-1 )

Gen-X adjusted

Gen-X pre-adjustment

Chandra

0.01 0.1 1

-11

-7

-9

-5

-13

Con-X goal

Gen-X axial PSDFrequency (cycles mm-1 )

•Begin with Con-X optic goal,

•2 cm axial actuators give figure correction < 0.025 mm- 1

I.e. Fourier low pass filter

•Correct to:

•6.5 nm rms 0.001<<0.01 mm-1

~ 2 times Con-X goal

•1.6 nm rms 0.01<<0.1 mm-1

~ 10 times Con-X goal

Page 12: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

12

Martin Elvis, Astrophysics 2020, 14 November 2007

PBM Development needed for X-ray Astronomy

• Thin replica substrates - bonding PBM• 2-D Wolter geometry

• axial + azimuthal curvature• Radiation hard piezo materials• Cold operation piezos • Getting the wires out

• Mass production: 100 m2 Aeff

104 m2 polished area• Cost• Speed - ~3 year production

• ~2x105 (2 cm actuators)/m2 Aeff :• Calibration• Calculation problem -

• closed loop essential in orbit

GRATING ASSEMBLY

INFLATIABLEINSTRUMENTSHIELD

SOLAR ARRAY

1.5M ANTENNA

SOLAR ARRAY

THERMAL COLLECTOR

THERMAL RADIATOR

INFLATABLE SUN SHIELD

Page 13: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

13

Martin Elvis, Astrophysics 2020, 14 November 2007

Active X-ray Optics:

A More Immediate Goal?

• ~50 times Con-X area is a big leap

• Chandra/Con-X ‘Hubble/Keck’ complementarity be lost after Chandra.

• Great Observatories IR/Opt/X diminished

• Budget future is always murky.

• Should we consider a small active X-ray optics mission before Gen-X?

• Mirror cost/speed advantage may not be so great for smaller diameter mirrors;

• Won’t reach 1st black holes;

• … but still more powerful than Chandra

Blind men and the elephant. Manga VIII Hokusai, Katsushika (1760-1849)

Page 14: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

14

Martin Elvis, Astrophysics 2020, 14 November 2007

Active X-ray OpticsActive X-ray OpticsFor The Next High Resolution X-ray Observatory

• Only way to go?

• Feasible: Piezoelectric Bimorph Mirrors address biggest technical challenge

• Development needed for telescope use

• Rapid development program could further all imaging X-ray astronomy missions

The Crab Nebula A Cosmic Synchrotron

Page 15: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

15

Martin Elvis, Astrophysics 2020, 14 November 2007

1600 200018001700 1900

0.1”

1”

10”

100”

Galileo1610

Hubble

Dawn of History

Optical Astronomy

X-r

ay A

stro

no

my

Chandra

From 0.5” to 0.1”, and on to the Diffraction limit <20masr

Ang

ular

res

olut

ion

Gen-X

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Active X-ray OpticsActive X-ray Opticsopens a new long-term vision for X-ray Astronomy

Page 16: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

16

Martin Elvis, Astrophysics 2020, 14 November 2007

Chandra: ~0.5”

The Supernova Remnant Cassiopeia A

ROSAT: ~5”

The Chandra Revolution:qualitatively new structures

Page 17: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

17

Martin Elvis, Astrophysics 2020, 14 November 2007

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

The Giant Galaxy M87 in the Virgo Cluster

Chandra only gives this Detail on the nearest of each Class of Celestial Object

ROSAT: ~5”

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Chandra: ~0.5”

Page 18: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

18

Martin Elvis, Astrophysics 2020, 14 November 2007

The Chandra X-ray ObservatorySub-arcsecond imaging by Chandra

has revolutionized astronomy

Page 19: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

19

Martin Elvis, Astrophysics 2020, 14 November 2007

High Resolution X-ray Optics for Astronomy: Challenging Requirements

Challenges

• Optical path clearance

• Sensing misalignments

• Calculating adjustments

• Applying corrections

• Stable actuators

Advantages• Reduced ground calibration• Reduced launch stability

requirements• Can operate away from room

temperature• Slow adjustments ~10-5 Hz high orbit

C.f. 10 Hz on ground-based telescopes

• High angular resolution, large area thin shells

• Axial figure errors comparable to Chandra

• Azimuthal figure errors substantially better

On-orbit adjustment of figure?

Page 20: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

20

Martin Elvis, Astrophysics 2020, 14 November 2007

Gen-X Study: Feasibility

2 options:

1. 125m f.l. Separate mirror detector s/c

2. 6 25m f.l., 8m dia mirrors

No show stoppers Launch capability to Sun-Earth L2 OK

Power budget OK

Main Challenge: Mirror technology 1/100 Chandra mass/area

10 x better angular resolution

GRATING ASSEMBLY

INFLATIABLEINSTRUMENTSHIELD

SOLAR ARRAY

1.5M ANTENNA

SOLAR ARRAY

THERMAL COLLECTOR

THERMAL RADIATOR

INFLATABLE SUN SHIELD

Page 21: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

21

Martin Elvis, Astrophysics 2020, 14 November 2007

Piezoelectric Bi-morph Mirrors (PBM):

Good Properties for Astronomy I• Thin: no optical path blockage

• Natural match to thin reflectors • 0.2 mm

• Low power, weight

• Existing synchrotron K-B mirrors comparable size to telescope segments

• Pairs of oppositely directed piezos remove T dependence

• Stable over days, months

• No anticlastic effect (‘saddling’)

Suzaku Mirror segment

Page 22: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

22

Martin Elvis, Astrophysics 2020, 14 November 2007

• Piezos parallel to mirror surface

• Reduce amplitude of errors by factor 15

• From 150 nm to 10 nm

• Factor 100 more improvement possible

• C.f. mechanical actuators:

No -

• Optical path blockage• lubricants • hysterisis• backlash

Piezoelectric Bi-morph Mirrors (PBM):

Good Properties for Astronomy IICitterio et al.

Page 23: 1 Martin Elvis, Astrophysics 2020, 14 November 2007 Active X-ray Optics For The Next High Resolution X-ray Observatory Martin Elvis Harvard-Smithsonian

23

Martin Elvis, Astrophysics 2020, 14 November 2007

Active X-ray Optics Alignment:

Signal & Compute Challenges

• 105 actuators! How to sense adjustments?

• Form defocussed image

Separate images of each shell, and azimuthal sector of parabola-hyperbola pair

• Factorizes calculation • Each shell segment, P-H pair is independent

• Separate P, H via finite focus source?

• Computation not overly demanding

Chandra Ring Focus Test

• Example: 20m dia mirror, 10cm actuators

• Annular images 400 mm thick: 20 resolved elements with 20 mm pixels