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Flat Exposure Properties of VIRCAM Detectors
https://people.ast.cam.ac.uk/~wfcam/docs/reports/vircam_flatreport/8 Dec 2006: 1.32 /- 0.05. 0.53 /- 0.01. 8. 2.23 /- 0.24. 0.61 /- 0.03. ... figure 5.10 Detector 10 (0.10%). figure 5.11 Detector 11 (0.24%). figure 5.12 Detector 12 (0.22%). -
Flat Exposure Properties of VIRCAM Detectors
https://people.ast.cam.ac.uk/~wfcam/docs/reports/vircam_flatreport/vircam_flatreport.html8 Dec 2006: 1.32 /- 0.05. 0.53 /- 0.01. 8. 2.23 /- 0.24. 0.61 /- 0.03. ... figure 5.10 Detector 10 (0.10%). figure 5.11 Detector 11 (0.24%). figure 5.12 Detector 12 (0.22%). -
42414.dvi
www-g.eng.cam.ac.uk/nms/publications/pdf/Bottani_EPL1998.pdf8 Dec 2006: Our results differ considerably from those reported in [24]. c. e. ... 24] Pailard V., Melinon P., Perez J. P., Dupuis V., Perez A., Loubet J. -
No Job Name
https://www2.mrc-lmb.cam.ac.uk/groups/JYL/PDF/MreC%20MM%202006.pdf7 Dec 2006: Plateswere incubated at 30C for 24–48 h, and any colour changewas noted. ... Curr Opin Cell Biol 16: 24–31. Barton, G.J. (1993) ALSCRIPT: a tool to format multiplesequence alignments. -
Particle Flow and ILC Detector Design
https://www.hep.phy.cam.ac.uk/~thomson/talks/ALCPG_Fermilab.pdf7 Dec 2006: gaps between Tungsten increase effective RMoliere)• Lateral segmentation: 1cm2 matched to RMoliere• Longitudinal segmentation: 30 layers (24 X0, 0.9λhad)• Typical resolution: σE/E = 0.15/E(GeV). ... ALCPG Seminar, Fermilab 8/12/2006 Mark Thomson -
Using APL format
www-g.eng.cam.ac.uk/nms/publications/pdf/Ilie_APL2000.pdf6 Dec 2006: Thepresence of a RamanD peak at;1350 cm21 indicates thatthe s p2 phase is clustering into aromatic rings.18 There is arelationship23,24 between the in-plane correlation lengthL a ofthe ... 2.24 I (D)/I (G) is derived from the Raman spectra -
USING STANDARD SYSTE
www-g.eng.cam.ac.uk/nms/publications/pdf/Ferrari_PRB2000b.pdf6 Dec 2006: Received 24 November 1999! The model and theoretical understanding of the Raman spectra in disordered and amorphous carbon aregiven. ... become localized.24 Olefinic CvCbonds are shorter than aromatic bonds, so they have hi. -
PII: S0925-9635(99)00271-X
www-g.eng.cam.ac.uk/nms/publications/pdf/Conway_DRM2000.pdf6 Dec 2006: decreases,E0 is measured at lower energies and no longer over a gap defects that could not be measured by ESR [ 24 ]. Robertson [ 25 ] demonstrated that it is possible to fit ... Robertson, Phys. Rev. B 53 (1996 ) 1594. [ 24 ] F. -
PII: S0925-9635(99)00245-9
www-g.eng.cam.ac.uk/nms/publications/pdf/Pastorelli_DRM2000.pdf6 Dec 2006: 85 (av.) 31.4 (av.) 3.24 63.5ta-C:H Homog. 70 28.4 2.35 70 6 30ta-C:H Homog 70 28.4 2.35 43 8.4 ... cm3and a internal layer 63.5 nm thick, with density of3.24 g/cm3[ 12]. -
PII: S0925-9635(99)00233-2
www-g.eng.cam.ac.uk/nms/publications/pdf/LiBassi_DRM2000.pdf6 Dec 2006: Diamond and Related Materials 9 (2000 ) 771–776www.elsevier.com/locate/diamond. Density, sp3 content and internal layering of DLC films byX-ray reflectivity and electron energy loss spectroscopy. A. LiBassi a, A.C. Ferrari b,, V. Stolojan c, B.K.
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