Diamond detectors for high energy physics

C. White; W. Dulinski; D. Fujino; K. K. Gan; R. Gilman; S. Han; J. Hassard; A. Howard; H. Kagan; S. Kanda; D. Kania; R. Kass; S. K. Kim; G. Kumbartski; M. H. Lee; K. Lister; R. Malchow; S. Margetides; L. S. Pan; P. Rutt; F. Sannes; S. Schnetzer; S. V. Somalwar; J. Straver; R. Stone; R. Tesarek; G. B. Thomson; W. Trischuk; Y. Sugimoto; G. B. Thomson; P. Weilhammer; C. White; S. Zhao

doi:10.1016/0168-9002(94)91082-0

Diamond detectors for high energy physics

C. White, W. Dulinski, D. Fujino, K. K. Gan, R. Gilman, S. Han, J. Hassard, A. Howard, H. Kagan, S. Kanda, D. Kania, R. Kass, S. K. Kim, G. Kumbartski, M. H. Lee, K. Lister, R. Malchow, S. Margetides, L. S. Pan, P. RuttF. Sannes, S. Schnetzer, S. V. Somalwar, J. Straver, R. Stone, R. Tesarek, G. B. Thomson, W. Trischuk, Y. Sugimoto, G. B. Thomson, P. Weilhammer, C. White, S. Zhao

School of Arts and Sciences, Physics & Astronomy

Research output: Contribution to journal › Article › peer-review

7 Scopus citations

Abstract

We have constructed charged particle detectors using high quality CVD diamond. We report here the measurements of a diamond-tungsten sampling calorimeter and a diamond mustrip detector. The energy response and resolution ( σ_E E) of the calorimeter were measured using an electron beam of energy 0.5 to 5.0 GeV, and compared with those from a silicon calorimeter of similar construction. We find σ_E E = (4.7 ± 2.7)%/E ⊕ (19.13 ± 0.86)%/√E ⊕ (2.3 ± 1.8)% for the diamond-tungsten calorimeter, where ⊕ indicates addition in quadrature, which is in good agreement with our result of σ_E/E = (3.89 ± 0.87)%/E ⊕ (19.73 ± 0.19)%/√E ⊕ (0.0 ± 1.6)% for the silicon-tungsten calorimeter. The CVD diamond mustrip detector consists of 50 μm wide strips on 100 μm centers. A signal-to-noise ratio of 6: 1 and a position resolution of 25 μm was observed during recent accelerator tests.

Original language	English (US)
Pages (from-to)	217-221
Number of pages	5
Journal	Nuclear Inst. and Methods in Physics Research, A
Volume	351
Issue number	1
DOIs	https://doi.org/10.1016/0168-9002(94)91082-0
State	Published - Nov 15 1994

All Science Journal Classification (ASJC) codes

Nuclear and High Energy Physics
Instrumentation

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10.1016/0168-9002(94)91082-0

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White, C., Dulinski, W., Fujino, D., Gan, K. K., Gilman, R., Han, S., Hassard, J., Howard, A., Kagan, H., Kanda, S., Kania, D., Kass, R., Kim, S. K., Kumbartski, G., Lee, M. H., Lister, K., Malchow, R., Margetides, S., Pan, L. S., ... Zhao, S. (1994). Diamond detectors for high energy physics. Nuclear Inst. and Methods in Physics Research, A, 351(1), 217-221. https://doi.org/10.1016/0168-9002(94)91082-0

@article{8abb329c68fa4ca4adc979feb1198efe,

title = "Diamond detectors for high energy physics",

abstract = "We have constructed charged particle detectors using high quality CVD diamond. We report here the measurements of a diamond-tungsten sampling calorimeter and a diamond mustrip detector. The energy response and resolution ( σE E) of the calorimeter were measured using an electron beam of energy 0.5 to 5.0 GeV, and compared with those from a silicon calorimeter of similar construction. We find σE E = (4.7 ± 2.7)%/E ⊕ (19.13 ± 0.86)%/√E ⊕ (2.3 ± 1.8)% for the diamond-tungsten calorimeter, where ⊕ indicates addition in quadrature, which is in good agreement with our result of σE/E = (3.89 ± 0.87)%/E ⊕ (19.73 ± 0.19)%/√E ⊕ (0.0 ± 1.6)% for the silicon-tungsten calorimeter. The CVD diamond mustrip detector consists of 50 μm wide strips on 100 μm centers. A signal-to-noise ratio of 6: 1 and a position resolution of 25 μm was observed during recent accelerator tests.",

author = "C. White and W. Dulinski and D. Fujino and Gan, {K. K.} and R. Gilman and S. Han and J. Hassard and A. Howard and H. Kagan and S. Kanda and D. Kania and R. Kass and Kim, {S. K.} and G. Kumbartski and Lee, {M. H.} and K. Lister and R. Malchow and S. Margetides and Pan, {L. S.} and P. Rutt and F. Sannes and S. Schnetzer and Somalwar, {S. V.} and J. Straver and R. Stone and R. Tesarek and Thomson, {G. B.} and W. Trischuk and Y. Sugimoto and Thomson, {G. B.} and P. Weilhammer and C. White and S. Zhao",

year = "1994",

month = nov,

day = "15",

doi = "10.1016/0168-9002(94)91082-0",

language = "English (US)",

volume = "351",

pages = "217--221",

journal = "Nuclear Inst. and Methods in Physics Research, A",

issn = "0168-9002",

publisher = "Elsevier",

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White, C, Dulinski, W, Fujino, D, Gan, KK, Gilman, R, Han, S, Hassard, J, Howard, A, Kagan, H, Kanda, S, Kania, D, Kass, R, Kim, SK, Kumbartski, G, Lee, MH, Lister, K, Malchow, R, Margetides, S, Pan, LS, Rutt, P, Sannes, F, Schnetzer, S , Somalwar, SV, Straver, J, Stone, R, Tesarek, R, Thomson, GB, Trischuk, W, Sugimoto, Y, Thomson, GB, Weilhammer, P, White, C & Zhao, S 1994, 'Diamond detectors for high energy physics', Nuclear Inst. and Methods in Physics Research, A, vol. 351, no. 1, pp. 217-221. https://doi.org/10.1016/0168-9002(94)91082-0

TY - JOUR

T1 - Diamond detectors for high energy physics

AU - White, C.

AU - Dulinski, W.

AU - Fujino, D.

AU - Gan, K. K.

AU - Gilman, R.

AU - Han, S.

AU - Hassard, J.

AU - Howard, A.

AU - Kagan, H.

AU - Kanda, S.

AU - Kania, D.

AU - Kass, R.

AU - Kim, S. K.

AU - Kumbartski, G.

AU - Lee, M. H.

AU - Lister, K.

AU - Malchow, R.

AU - Margetides, S.

AU - Pan, L. S.

AU - Rutt, P.

AU - Sannes, F.

AU - Schnetzer, S.

AU - Somalwar, S. V.

AU - Straver, J.

AU - Stone, R.

AU - Tesarek, R.

AU - Thomson, G. B.

AU - Trischuk, W.

AU - Sugimoto, Y.

AU - Thomson, G. B.

AU - Weilhammer, P.

AU - White, C.

AU - Zhao, S.

PY - 1994/11/15

Y1 - 1994/11/15

N2 - We have constructed charged particle detectors using high quality CVD diamond. We report here the measurements of a diamond-tungsten sampling calorimeter and a diamond mustrip detector. The energy response and resolution ( σE E) of the calorimeter were measured using an electron beam of energy 0.5 to 5.0 GeV, and compared with those from a silicon calorimeter of similar construction. We find σE E = (4.7 ± 2.7)%/E ⊕ (19.13 ± 0.86)%/√E ⊕ (2.3 ± 1.8)% for the diamond-tungsten calorimeter, where ⊕ indicates addition in quadrature, which is in good agreement with our result of σE/E = (3.89 ± 0.87)%/E ⊕ (19.73 ± 0.19)%/√E ⊕ (0.0 ± 1.6)% for the silicon-tungsten calorimeter. The CVD diamond mustrip detector consists of 50 μm wide strips on 100 μm centers. A signal-to-noise ratio of 6: 1 and a position resolution of 25 μm was observed during recent accelerator tests.

AB - We have constructed charged particle detectors using high quality CVD diamond. We report here the measurements of a diamond-tungsten sampling calorimeter and a diamond mustrip detector. The energy response and resolution ( σE E) of the calorimeter were measured using an electron beam of energy 0.5 to 5.0 GeV, and compared with those from a silicon calorimeter of similar construction. We find σE E = (4.7 ± 2.7)%/E ⊕ (19.13 ± 0.86)%/√E ⊕ (2.3 ± 1.8)% for the diamond-tungsten calorimeter, where ⊕ indicates addition in quadrature, which is in good agreement with our result of σE/E = (3.89 ± 0.87)%/E ⊕ (19.73 ± 0.19)%/√E ⊕ (0.0 ± 1.6)% for the silicon-tungsten calorimeter. The CVD diamond mustrip detector consists of 50 μm wide strips on 100 μm centers. A signal-to-noise ratio of 6: 1 and a position resolution of 25 μm was observed during recent accelerator tests.

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U2 - 10.1016/0168-9002(94)91082-0

DO - 10.1016/0168-9002(94)91082-0

M3 - Article

AN - SCOPUS:0028538503

SN - 0168-9002

VL - 351

SP - 217

EP - 221

JO - Nuclear Inst. and Methods in Physics Research, A

JF - Nuclear Inst. and Methods in Physics Research, A

IS - 1

ER -

Diamond detectors for high energy physics

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