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Dive into the research topics where Martin Nordby is active.

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Featured researches published by Martin Nordby.


Proceedings of SPIE | 2012

The CSPAD megapixel x-ray camera at LCLS

P. Hart; Sébastien Boutet; G. A. Carini; Mikhail Dubrovin; B. Duda; David M. Fritz; G. Haller; R. Herbst; Sven Herrmann; Chris Kenney; N. Kurita; Henrik T. Lemke; Marc Messerschmidt; Martin Nordby; J. Pines; Don Schafer; Matt Swift; M. Weaver; Garth J. Williams; Diling Zhu; Niels van Bakel; John Morse

The Linear Coherent Light Source (LCLS), a free electron laser operating from 250eV to10keV at 120Hz, is opening windows on new science in biology, chemistry, and solid state, atomic, and plasma physics1,2. The FEL provides coherent x-rays in femtosecond pulses of unprecedented intensity. This allows the study of materials on up to 3 orders of magnitude shorter time scales than previously possible. Many experiments at the LCLS require a detector that can image scattered x-rays on a per-shot basis with high efficiency and excellent spatial resolution over a large solid angle and both good S/N (for single-photon counting) and large dynamic range (required for the new coherent x-ray diffractive imaging technique3). The Cornell-SLAC Pixel Array Detector (CSPAD) has been developed to meet these requirements. SLAC has built, characterized, and installed three full camera systems at the CXI and XPP hutches at LCLS. This paper describes the camera system and its characterization and performance.


nuclear science symposium and medical imaging conference | 2012

The Cornell-SLAC pixel array detector at LCLS

P. Hart; Sébastien Boutet; G. CarmI; A. Dragone; B. Duda; D. Freytag; G. Haller; R. Herbst; S. Herrmann; C. J. Kenney; John Morse; Martin Nordby; J. Pines; N. van Bakel; M. Weaver; Garth J. Williams

The Cornell-SLAC pixel array detector (CSpad) is a general-purpose integrating hybrid pixel x-ray camera developed for use at the Linear Coherent Light Source (LCLS) x-ray free electron laser at the SLAC National Accelerator Laboratory (SLAC). The detector has a full well capacity of about 2.Sk photons in low-gain mode and a SIN of about 6 in high-gain mode. Its 2.3M pixels are read out at 120 Hz. The detector comprises 32 500μm silicon sensors bump-bonded to 64 185×194-pixel ASICs. The pixel size is 110μm. The water-cooled detector quadrants can be radially moved in-situ to vary the beam aperture. SLAC has built, calibrated, and optimized three complete camera systems based on a sensor and ASIC designed by Cornell. The camera is read out by a DAQ system which provides extensive online monitoring and prompt analysis capabilities. We have also built a dozen smaller cameras in a portable form-factor for use in confined spaces and for ease of development, testing, and deployment. Through 2012 user experiments have taken almost a petabyte of data with these detectors in a variety of applications. We have extensively tested the detector at synchrotrons and with an x-ray tube, in addition to commissioning tests at the LCLS, investigating linearity, cross-talk, homogeneity, and radiation hardness. The SLAC detector group is deploying improved support infrastructure and an updated ASIC and electronics based on this experience. This paper describes the instrument, its calibration and performance, and presents preliminary results from the updated camera.


ieee particle accelerator conference | 1997

Results from a prototype permanent magnet dipole-quadrupole hybrid for the PEP-II B-factory

M. Sullivan; G. Bowden; S. Ecklund; D. Jensen; Martin Nordby; A. Ringwall; Z. R. Wolf

We describe the construction of a prototype hybrid permanent magnet dipole and quadrupole. The magnet consists of two concentric rings of Sm/sub 2/Co/sub 17/ magnetic material 5 cm in length. The outer ring is made of 16 uniformly magnetized blocks assembled as a Halbach dipole and the inner ring has 32 blocks oriented in a similar fashion so as to generate a quadrupole field. The resultant superimposed field is an offset quadrupole field which allows us to center the field on the high-energy beam in the interaction region of the PEP-II B-factory. The dipole blocks are glued to the inside surface of an outer support collar and the quadrupole blocks are held in a fixture that allows radial adjustment of the blocks prior to potting the entire assembly with epoxy. An extensive computer model of the magnet has been made and from this model we developed a tuning algorithm that allowed us to greatly reduce the n=3-17 harmonics of the magnet.


ieee particle accelerator conference | 1995

Bellows design for the PEP-II High Energy Ring arc chambers

Martin Nordby; N. Kurita; C.-K. Ng

An overview of the current bellows module design and performance parameters is presented. Performance requirements based on external chamber design constraints, and operational needs are discussed. Parameters include beam impedance of the RF shield, and electrical resistance of the shield gap joint. Also discussed is the analysis of the high-current thermal management, and structural and cyclic behavior of the bellows and RF shield. Experiments of the tribology and electrical resistance of the shield sliding joint are summarized, and their results presented. Existing and new design options are discussed in light of the analyses and experiments. The final design is presented as the optimal compromise between the varying parameters.


Proceedings of SPIE | 2010

Using SysML for MBSE analysis of the LSST system

Charles F. Claver; Gregory P. Dubois-Felsmann; Francisco Delgado; Pat Hascall; S. L. Marshall; Martin Nordby; Terry Schalk; German Schumacher; Jacques Sebag

The Large Synoptic Survey Telescope is a complex hardware - software system of systems, making up a highly automated observatory in the form of an 8.4m wide-field telescope, a 3.2 billion pixel camera, and a peta-scale data processing and archiving system. As a project, the LSST is using model based systems engineering (MBSE) methodology for developing the overall system architecture coded with the Systems Modeling Language (SysML). With SysML we use a recursive process to establish three-fold relationships between requirements, logical & physical structural component definitions, and overall behavior (activities and sequences) at successively deeper levels of abstraction and detail. Using this process we have analyzed and refined the LSST system design, ensuring the consistency and completeness of the full set of requirements and their match to associated system structure and behavior. As the recursion process proceeds to deeper levels we derive more detailed requirements and specifications, and ensure their traceability. We also expose, define, and specify critical system interfaces, physical and information flows, and clarify the logic and control flows governing system behavior. The resulting integrated model database is used to generate documentation and specifications and will evolve to support activities from construction through final integration, test, and commissioning, serving as a living representation of the LSST as designed and built. We discuss the methodology and present several examples of its application to specific systems engineering challenges in the LSST design.


Proceedings Particle Accelerator Conference | 1995

The vacuum system for the PEP II High Energy Ring straight sections

U. Wienands; E. Daly; S. Heifets; A. Kulikov; N. Kurita; Martin Nordby; C. Perkins; E. Reuter; J. Seeman; F.C. Belser; J. Berg; F.R. Holdener; J.A. Kerns; M.R. McDaniel; W. Stoeffl

The six straight insertions of the PEP II High Energy Ring (HER) serve various functions: lattice tuning, beam injection and abort, providing space for RF cavities, longitudinal and transverse feedback, beam diagnostics and the interaction point. A stainless steel vacuum system has been designed; prototypes are currently being built. Cooling is required due to radiation coming from the last arc dipole and resistive losses in the vacuum chamber. Although the nominal beam current of the HER is 1 A the vacuum system is designed for 3 A to provide margin and an upgrade path.


Proceedings of SPIE | 2012

LSST camera optics design

Scot S. Olivier; Vincent J. Riot; David K. Gilmore; Brian J. Bauman; Steve Pratuch; Lynn G. Seppala; John Ku; Martin Nordby; Mike Foss; P. Antilogus; N. Morgado; B. Sassolas; R. Flaminio; C. Michel

The Large Synoptic Survey Telescope (LSST) uses a novel, three-mirror, telescope design feeding a camera system that includes a set of broad-band filters and three refractive corrector lenses to produce a flat field at the focal plane with a wide field of view. Optical design of the camera lenses and filters is integrated in with the optical design of telescope mirrors to optimize performance. We discuss the rationale for the LSST camera optics design, describe the methodology for fabricating, coating, mounting and testing the lenses and filters, and present the results of detailed analyses demonstrating that the camera optics will meet their performance goals.


Proceedings of SPIE | 2008

The LSST camera overview: design and performance

Kirk Gilmore; Steven M. Kahn; Martin Nordby; Paul O'Connor; J. Oliver; V. Radeka; Terry Schalk; R. Schindler; Rick Van Berg

The LSST camera is a wide-field optical (0.35-1μm) imager designed to provide a 3.5 degree FOV with 0.2 arcsecond/pixel sampling. The detector format will be a circular mosaic providing approximately 3.2 Gigapixels per image. The camera includes a filter mechanism and shuttering capability. It is positioned in the middle of the telescope where cross-sectional area is constrained by optical vignetting and where heat dissipation must be controlled to limit thermal gradients in the optical beam. The fast f/1.2 beam will require tight tolerances on the focal plane mechanical assembly. The focal plane array operates at a temperature of approximately -100°C to achieve desired detector performance. The focal plane array is contained within a cryostat which incorporates detector front-end electronics and thermal control. The cryostat lens serves as an entrance window and vacuum seal for the cryostat. Similarly, the camera body lens serves as an entrance window and gas seal for the camera housing, which is filled with a suitable gas to provide the operating environment for the shutter and filter change mechanisms. The filter carousel accommodates 5 filters, each 75 cm in diameter, for rapid exchange without external intervention.


Proceedings of SPIE | 2008

Mechanical design of the LSST camera

Martin Nordby; Gordon Bowden; Mike Foss; Gary Guiffre; John Ku; R. Schindler

The LSST camera is a tightly packaged, hermetically-sealed system that is cantilevered into the main beam of the LSST telescope. It is comprised of three refractive lenses, on-board storage for five large filters, a high-precision shutter, and a cryostat that houses the 3.2 giga-pixel CCD focal plane along with its support electronics. The physically large optics and focal plane demand large structural elements to support them, but the overall size of the camera and its components must be minimized to reduce impact on the image stability. Also, focal plane and optics motions must be minimized to reduce systematic errors in image reconstruction. Design and analysis for the camera body and cryostat will be detailed.


Proceedings of SPIE | 2006

The LSST camera system overview

Kirk Gilmore; Steven M. Kahn; Martin Nordby; David L. Burke; Paul O'Connor; J. Oliver; V. Radeka; Terry Schalk; R. Schindler

The LSST camera is a wide-field optical (0.35-1um) imager designed to provide a 3.5 degree FOV with better than 0.2 arcsecond sampling. The detector format will be a circular mosaic providing approximately 3.2 Gigapixels per image. The camera includes a filter mechanism and, shuttering capability. It is positioned in the middle of the telescope where cross-sectional area is constrained by optical vignetting and heat dissipation must be controlled to limit thermal gradients in the optical beam. The fast, f/1.2 beam will require tight tolerances on the focal plane mechanical assembly. The focal plane array operates at a temperature of approximately -100°C to achieve desired detector performance. The focal plane array is contained within an evacuated cryostat, which incorporates detector front-end electronics and thermal control. The cryostat lens serves as an entrance window and vacuum seal for the cryostat. Similarly, the camera body lens serves as an entrance window and gas seal for the camera housing, which is filled with a suitable gas to provide the operating environment for the shutter and filter change mechanisms. The filter carousel can accommodate 5 filters, each 75 cm in diameter, for rapid exchange without external intervention.

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R. Schindler

SLAC National Accelerator Laboratory

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Terry Schalk

University of California

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Steven M. Kahn

University of California

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Paul O'Connor

Brookhaven National Laboratory

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V. Radeka

Brookhaven National Laboratory

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