The Muonic Hydrogen Lamb Shift Experiment at PSI
Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the...
Ausführliche Beschreibung
Autor*in: |
Kottmann, F. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2001 |
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Schlagwörter: |
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Anmerkung: |
© Kluwer Academic Publishers 2001 |
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Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 138(2001), 1-4 vom: Dez., Seite 55-60 |
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Übergeordnetes Werk: |
volume:138 ; year:2001 ; number:1-4 ; month:12 ; pages:55-60 |
Links: |
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DOI / URN: |
10.1023/A:1020886314237 |
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Katalog-ID: |
OLC2076400907 |
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520 | |a Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. | ||
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650 | 4 | |a Muonic Hydrogen | |
700 | 1 | |a Amir, W. |4 aut | |
700 | 1 | |a Biraben, F. |4 aut | |
700 | 1 | |a Conde, C. A. N. |4 aut | |
700 | 1 | |a Dhawan, S. |4 aut | |
700 | 1 | |a Hänsch, T. W. |4 aut | |
700 | 1 | |a Hartmann, F. J. |4 aut | |
700 | 1 | |a Hughes, V. W. |4 aut | |
700 | 1 | |a Huot, O. |4 aut | |
700 | 1 | |a Indelicato, P. |4 aut | |
700 | 1 | |a Julien, L. |4 aut | |
700 | 1 | |a Knowles, P. |4 aut | |
700 | 1 | |a Kazamias, S. |4 aut | |
700 | 1 | |a Liu, Y.-W. |4 aut | |
700 | 1 | |a Mulhauser, F. |4 aut | |
700 | 1 | |a Nez, F. |4 aut | |
700 | 1 | |a Pohl, R. |4 aut | |
700 | 1 | |a Rabinowitz, P. |4 aut | |
700 | 1 | |a dos Santos, J. M. F. |4 aut | |
700 | 1 | |a Schaller, L. A. |4 aut | |
700 | 1 | |a Schneuwly, H. |4 aut | |
700 | 1 | |a Schott, W. |4 aut | |
700 | 1 | |a Taqqu, D. |4 aut | |
700 | 1 | |a Veloso, J. F. C. A. |4 aut | |
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10.1023/A:1020886314237 doi (DE-627)OLC2076400907 (DE-He213)A:1020886314237-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kottmann, F. verfasserin aut The Muonic Hydrogen Lamb Shift Experiment at PSI 2001 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 2001 Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. Vacuum Polarization Lamb Shift Paul Scherrer Institute Muon Beam Muonic Hydrogen Amir, W. aut Biraben, F. aut Conde, C. A. N. aut Dhawan, S. aut Hänsch, T. W. aut Hartmann, F. J. aut Hughes, V. W. aut Huot, O. aut Indelicato, P. aut Julien, L. aut Knowles, P. aut Kazamias, S. aut Liu, Y.-W. aut Mulhauser, F. aut Nez, F. aut Pohl, R. aut Rabinowitz, P. aut dos Santos, J. M. F. aut Schaller, L. A. aut Schneuwly, H. aut Schott, W. aut Taqqu, D. aut Veloso, J. F. C. A. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 138(2001), 1-4 vom: Dez., Seite 55-60 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:138 year:2001 number:1-4 month:12 pages:55-60 https://doi.org/10.1023/A:1020886314237 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 138 2001 1-4 12 55-60 |
spelling |
10.1023/A:1020886314237 doi (DE-627)OLC2076400907 (DE-He213)A:1020886314237-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kottmann, F. verfasserin aut The Muonic Hydrogen Lamb Shift Experiment at PSI 2001 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 2001 Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. Vacuum Polarization Lamb Shift Paul Scherrer Institute Muon Beam Muonic Hydrogen Amir, W. aut Biraben, F. aut Conde, C. A. N. aut Dhawan, S. aut Hänsch, T. W. aut Hartmann, F. J. aut Hughes, V. W. aut Huot, O. aut Indelicato, P. aut Julien, L. aut Knowles, P. aut Kazamias, S. aut Liu, Y.-W. aut Mulhauser, F. aut Nez, F. aut Pohl, R. aut Rabinowitz, P. aut dos Santos, J. M. F. aut Schaller, L. A. aut Schneuwly, H. aut Schott, W. aut Taqqu, D. aut Veloso, J. F. C. A. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 138(2001), 1-4 vom: Dez., Seite 55-60 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:138 year:2001 number:1-4 month:12 pages:55-60 https://doi.org/10.1023/A:1020886314237 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 138 2001 1-4 12 55-60 |
allfields_unstemmed |
10.1023/A:1020886314237 doi (DE-627)OLC2076400907 (DE-He213)A:1020886314237-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kottmann, F. verfasserin aut The Muonic Hydrogen Lamb Shift Experiment at PSI 2001 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 2001 Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. Vacuum Polarization Lamb Shift Paul Scherrer Institute Muon Beam Muonic Hydrogen Amir, W. aut Biraben, F. aut Conde, C. A. N. aut Dhawan, S. aut Hänsch, T. W. aut Hartmann, F. J. aut Hughes, V. W. aut Huot, O. aut Indelicato, P. aut Julien, L. aut Knowles, P. aut Kazamias, S. aut Liu, Y.-W. aut Mulhauser, F. aut Nez, F. aut Pohl, R. aut Rabinowitz, P. aut dos Santos, J. M. F. aut Schaller, L. A. aut Schneuwly, H. aut Schott, W. aut Taqqu, D. aut Veloso, J. F. C. A. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 138(2001), 1-4 vom: Dez., Seite 55-60 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:138 year:2001 number:1-4 month:12 pages:55-60 https://doi.org/10.1023/A:1020886314237 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 138 2001 1-4 12 55-60 |
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10.1023/A:1020886314237 doi (DE-627)OLC2076400907 (DE-He213)A:1020886314237-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kottmann, F. verfasserin aut The Muonic Hydrogen Lamb Shift Experiment at PSI 2001 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 2001 Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. Vacuum Polarization Lamb Shift Paul Scherrer Institute Muon Beam Muonic Hydrogen Amir, W. aut Biraben, F. aut Conde, C. A. N. aut Dhawan, S. aut Hänsch, T. W. aut Hartmann, F. J. aut Hughes, V. W. aut Huot, O. aut Indelicato, P. aut Julien, L. aut Knowles, P. aut Kazamias, S. aut Liu, Y.-W. aut Mulhauser, F. aut Nez, F. aut Pohl, R. aut Rabinowitz, P. aut dos Santos, J. M. F. aut Schaller, L. A. aut Schneuwly, H. aut Schott, W. aut Taqqu, D. aut Veloso, J. F. C. A. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 138(2001), 1-4 vom: Dez., Seite 55-60 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:138 year:2001 number:1-4 month:12 pages:55-60 https://doi.org/10.1023/A:1020886314237 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 138 2001 1-4 12 55-60 |
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10.1023/A:1020886314237 doi (DE-627)OLC2076400907 (DE-He213)A:1020886314237-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kottmann, F. verfasserin aut The Muonic Hydrogen Lamb Shift Experiment at PSI 2001 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 2001 Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. Vacuum Polarization Lamb Shift Paul Scherrer Institute Muon Beam Muonic Hydrogen Amir, W. aut Biraben, F. aut Conde, C. A. N. aut Dhawan, S. aut Hänsch, T. W. aut Hartmann, F. J. aut Hughes, V. W. aut Huot, O. aut Indelicato, P. aut Julien, L. aut Knowles, P. aut Kazamias, S. aut Liu, Y.-W. aut Mulhauser, F. aut Nez, F. aut Pohl, R. aut Rabinowitz, P. aut dos Santos, J. M. F. aut Schaller, L. A. aut Schneuwly, H. aut Schott, W. aut Taqqu, D. aut Veloso, J. F. C. A. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 138(2001), 1-4 vom: Dez., Seite 55-60 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:138 year:2001 number:1-4 month:12 pages:55-60 https://doi.org/10.1023/A:1020886314237 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 138 2001 1-4 12 55-60 |
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Kottmann, F. @@aut@@ Amir, W. @@aut@@ Biraben, F. @@aut@@ Conde, C. A. N. @@aut@@ Dhawan, S. @@aut@@ Hänsch, T. W. @@aut@@ Hartmann, F. J. @@aut@@ Hughes, V. W. @@aut@@ Huot, O. @@aut@@ Indelicato, P. @@aut@@ Julien, L. @@aut@@ Knowles, P. @@aut@@ Kazamias, S. @@aut@@ Liu, Y.-W. @@aut@@ Mulhauser, F. @@aut@@ Nez, F. @@aut@@ Pohl, R. @@aut@@ Rabinowitz, P. @@aut@@ dos Santos, J. M. F. @@aut@@ Schaller, L. A. @@aut@@ Schneuwly, H. @@aut@@ Schott, W. @@aut@@ Taqqu, D. @@aut@@ Veloso, J. F. C. A. @@aut@@ |
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Kottmann, F. Amir, W. Biraben, F. Conde, C. A. N. Dhawan, S. Hänsch, T. W. Hartmann, F. J. Hughes, V. W. Huot, O. Indelicato, P. Julien, L. Knowles, P. Kazamias, S. Liu, Y.-W. Mulhauser, F. Nez, F. Pohl, R. Rabinowitz, P. dos Santos, J. M. F. Schaller, L. A. Schneuwly, H. Schott, W. Taqqu, D. Veloso, J. F. C. A. |
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the muonic hydrogen lamb shift experiment at psi |
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The Muonic Hydrogen Lamb Shift Experiment at PSI |
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Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. © Kluwer Academic Publishers 2001 |
abstractGer |
Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. © Kluwer Academic Publishers 2001 |
abstract_unstemmed |
Abstract A measurement of the 2S Lamb shift in muonic hydrogen ($ μ^{−} $p) is being prepared at the Paul Scherrer Institute (PSI). The goal of the experiment is to measure the energy difference ΔE($ 2^{5} $P3/2−$ 2^{3} $S1/2) by laser spectroscopy (λ≈6μm) to a precision of 30 ppm and to deduce the root mean square (rms) proton charge radius with $ 10^{−3} $ relative accuracy, 20 times more precise than presently known. An important prerequisite to this experiment is the availability of long-lived $ μp_{2S} $-atoms. A 2S-lifetime of ∼1 μs – sufficiently long to perform the laser experiment – at $ H_{2} $ gas pressures of 1–2 hPa was deduced from recent measurements of the collisional 2S-quenching rate. A new low-energy negative muon beam yields an order of magnitude more muon stops in a small low-density gas volume than a conventional cloud muon beam. A stack of ultra-thin carbon foils is the key element of a fast detector for keV-muons. The development of a 2 keV X-ray detector and a 3-stage laser system providing 0.5 mJ laser pulses at 6 μm is on the way. © Kluwer Academic Publishers 2001 |
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