Cargando…

Measurement of $K_{e3}^{0}$ form factors

The semi-leptonic decay of the neutral K meson $K^{0}_{L} \to \pi^{\pm}e^{\mp}\nu (K_{e3})$, was used to study the strangeness-changing weak interaction of hadrons. A sample of 5.6 million reconstructed events recorded by the NA48 experiment was used to measure the Dalitz plot density. Admitting all...

Descripción completa

Detalles Bibliográficos
Autores principales: Lai, A., Marras, D., Bevan, A., Dosanjh, R.S., Gershon, T.J., Hay, B., Kalmus, G.E., Lazzeroni, C., Munday, D.J., Olaiya, E., Parker, Michael Andrew, White, T.O., Wotton, S.A., Barr, G., Bocquet, G., Ceccucci, A., Cuhadar-Donszelmann, T., Cundy, D., D'Agostini, G., Doble, N., Falaleev, V., Gatignon, L., Gonidec, A., Gorini, B., Govi, G., Grafstrom, P., Kubischta, W., Lacourt, A., Norton, A., Palestini, S., Panzer-Steindel, B., Taureg, H., Velasco, M., Wahl, Heinrich, Cheshkov, C., Hristov, P., Kekelidze, V., Litov, L., Madigojine, D., Molokanova, N., Potrebenikov, Yu., Stoynev, S., Zinchenko, A., Knowles, I., Martin, V., Sacco, R., Walker, A., Contalbrigo, M., Dalpiaz, P., Duclos, J., Frabetti, P.L., Gianoli, A., Martini, M., Petrucci, F., Savrie, M., Bizzeti, A., Calvetti, M., Collazuol, G., Graziani, G., Iacopini, E., Lenti, M., Martelli, F., Veltri, M., Becker, H.G., Eppard, K., Eppard, M., Fox, H., Kalter, A., Kleinknecht, K., Koch, U., Kopke, L., Lopes da Silva, P., Marouelli, P., Pellmann, I., Peters, A., Renk, B., Schmidt, S.A., Schonharting, V., Schue, Y., Wanke, R., Winhart, A., Wittgen, M., Chollet, J.C., Fayard, L., Iconomidou-Fayard, L., Ocariz, J., Unal, G., Wingerter-Seez, I., Anzivino, G., Cenci, P., Imbergamo, E., Lubrano, P., Mestvirishvili, A., Nappi, A., Pepe, M., Piccini, M., Bertanza, L., Carosi, R., Casali, R., Cerri, C., Cirilli, M., Costantini, F., Fantechi, R., Giudici, S., Mannelli, I., Pierazzini, G., Sozzi, M., Cheze, J.B., Cogan, J., De Beer, M., Debu, P., Formica, A., Granier de Cassagnac, R., Mazzucato, E., Peyaud, B., Turlay, R., Vallage, B., Holder, M., Maier, A., Ziolkowski, M., Arcidiacono, R., Biino, C., Cartiglia, N., Marchetto, F., Menichetti, Ezio A., Pastrone, N., Nassalski, J., Rondio, E., Szleper, M., Wislicki, W., Wronka, S., Dibon, H., Fischer, G., Jeitler, M., Markytan, M., Mikulec, I., Neuhofer, G., Pernicka, M., Taurok, A., Widhalm, L.
Lenguaje:eng
Publicado: 2004
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2004.08.076
http://cds.cern.ch/record/798021
_version_ 1780904694697164800
author Lai, A.
Marras, D.
Bevan, A.
Dosanjh, R.S.
Gershon, T.J.
Hay, B.
Kalmus, G.E.
Lazzeroni, C.
Munday, D.J.
Olaiya, E.
Parker, Michael Andrew
White, T.O.
Wotton, S.A.
Barr, G.
Bocquet, G.
Ceccucci, A.
Cuhadar-Donszelmann, T.
Cundy, D.
D'Agostini, G.
Doble, N.
Falaleev, V.
Gatignon, L.
Gonidec, A.
Gorini, B.
Govi, G.
Grafstrom, P.
Kubischta, W.
Lacourt, A.
Norton, A.
Palestini, S.
Panzer-Steindel, B.
Taureg, H.
Velasco, M.
Wahl, Heinrich
Cheshkov, C.
Hristov, P.
Kekelidze, V.
Litov, L.
Madigojine, D.
Molokanova, N.
Potrebenikov, Yu.
Stoynev, S.
Zinchenko, A.
Knowles, I.
Martin, V.
Sacco, R.
Walker, A.
Contalbrigo, M.
Dalpiaz, P.
Duclos, J.
Frabetti, P.L.
Gianoli, A.
Martini, M.
Petrucci, F.
Savrie, M.
Bizzeti, A.
Calvetti, M.
Collazuol, G.
Graziani, G.
Iacopini, E.
Lenti, M.
Martelli, F.
Veltri, M.
Becker, H.G.
Eppard, K.
Eppard, M.
Fox, H.
Kalter, A.
Kleinknecht, K.
Koch, U.
Kopke, L.
Lopes da Silva, P.
Marouelli, P.
Pellmann, I.
Peters, A.
Renk, B.
Schmidt, S.A.
Schonharting, V.
Schue, Y.
Wanke, R.
Winhart, A.
Wittgen, M.
Chollet, J.C.
Fayard, L.
Iconomidou-Fayard, L.
Ocariz, J.
Unal, G.
Wingerter-Seez, I.
Anzivino, G.
Cenci, P.
Imbergamo, E.
Lubrano, P.
Mestvirishvili, A.
Nappi, A.
Pepe, M.
Piccini, M.
Bertanza, L.
Carosi, R.
Casali, R.
Cerri, C.
Cirilli, M.
Costantini, F.
Fantechi, R.
Giudici, S.
Mannelli, I.
Pierazzini, G.
Sozzi, M.
Cheze, J.B.
Cogan, J.
De Beer, M.
Debu, P.
Formica, A.
Granier de Cassagnac, R.
Mazzucato, E.
Peyaud, B.
Turlay, R.
Vallage, B.
Holder, M.
Maier, A.
Ziolkowski, M.
Arcidiacono, R.
Biino, C.
Cartiglia, N.
Marchetto, F.
Menichetti, Ezio A.
Pastrone, N.
Nassalski, J.
Rondio, E.
Szleper, M.
Wislicki, W.
Wronka, S.
Dibon, H.
Fischer, G.
Jeitler, M.
Markytan, M.
Mikulec, I.
Neuhofer, G.
Pernicka, M.
Taurok, A.
Widhalm, L.
author_facet Lai, A.
Marras, D.
Bevan, A.
Dosanjh, R.S.
Gershon, T.J.
Hay, B.
Kalmus, G.E.
Lazzeroni, C.
Munday, D.J.
Olaiya, E.
Parker, Michael Andrew
White, T.O.
Wotton, S.A.
Barr, G.
Bocquet, G.
Ceccucci, A.
Cuhadar-Donszelmann, T.
Cundy, D.
D'Agostini, G.
Doble, N.
Falaleev, V.
Gatignon, L.
Gonidec, A.
Gorini, B.
Govi, G.
Grafstrom, P.
Kubischta, W.
Lacourt, A.
Norton, A.
Palestini, S.
Panzer-Steindel, B.
Taureg, H.
Velasco, M.
Wahl, Heinrich
Cheshkov, C.
Hristov, P.
Kekelidze, V.
Litov, L.
Madigojine, D.
Molokanova, N.
Potrebenikov, Yu.
Stoynev, S.
Zinchenko, A.
Knowles, I.
Martin, V.
Sacco, R.
Walker, A.
Contalbrigo, M.
Dalpiaz, P.
Duclos, J.
Frabetti, P.L.
Gianoli, A.
Martini, M.
Petrucci, F.
Savrie, M.
Bizzeti, A.
Calvetti, M.
Collazuol, G.
Graziani, G.
Iacopini, E.
Lenti, M.
Martelli, F.
Veltri, M.
Becker, H.G.
Eppard, K.
Eppard, M.
Fox, H.
Kalter, A.
Kleinknecht, K.
Koch, U.
Kopke, L.
Lopes da Silva, P.
Marouelli, P.
Pellmann, I.
Peters, A.
Renk, B.
Schmidt, S.A.
Schonharting, V.
Schue, Y.
Wanke, R.
Winhart, A.
Wittgen, M.
Chollet, J.C.
Fayard, L.
Iconomidou-Fayard, L.
Ocariz, J.
Unal, G.
Wingerter-Seez, I.
Anzivino, G.
Cenci, P.
Imbergamo, E.
Lubrano, P.
Mestvirishvili, A.
Nappi, A.
Pepe, M.
Piccini, M.
Bertanza, L.
Carosi, R.
Casali, R.
Cerri, C.
Cirilli, M.
Costantini, F.
Fantechi, R.
Giudici, S.
Mannelli, I.
Pierazzini, G.
Sozzi, M.
Cheze, J.B.
Cogan, J.
De Beer, M.
Debu, P.
Formica, A.
Granier de Cassagnac, R.
Mazzucato, E.
Peyaud, B.
Turlay, R.
Vallage, B.
Holder, M.
Maier, A.
Ziolkowski, M.
Arcidiacono, R.
Biino, C.
Cartiglia, N.
Marchetto, F.
Menichetti, Ezio A.
Pastrone, N.
Nassalski, J.
Rondio, E.
Szleper, M.
Wislicki, W.
Wronka, S.
Dibon, H.
Fischer, G.
Jeitler, M.
Markytan, M.
Mikulec, I.
Neuhofer, G.
Pernicka, M.
Taurok, A.
Widhalm, L.
author_sort Lai, A.
collection CERN
description The semi-leptonic decay of the neutral K meson $K^{0}_{L} \to \pi^{\pm}e^{\mp}\nu (K_{e3})$, was used to study the strangeness-changing weak interaction of hadrons. A sample of 5.6 million reconstructed events recorded by the NA48 experiment was used to measure the Dalitz plot density. Admitting all possible Lorentz-covariant couplings, the form factors for vector $(f_{+}(q^{2}))$, scalar $(f_{S})$ and tensor $(f_{T})$ interactions were measured. The linear slope of the vector form factor $\lambda_{+} = 0.0284 \pm 0.0007 \pm 0.0013$ and values for the ratios $|f_{S}/f_{+}(0)|=0.015^{+0.007}_{-0.010} \pm 0.012$ and $|f_{T}/f_{+}(0)|=0.05^{+0.03}_{-0.04} \pm 0.03$ were obtained. The values for $f_{S}$ and for $f_{T}$ are consistent with zero. Assuming only vector-axial vector couplings, $\lambda_{+} = 0.02888 \pm 0.0004 \pm 0.0011$ and a good fit consistent with pure V-A couplings were obtained. Alternatively a fit to a dipole form factor yields a pole mass of $M = 859 \pm 18$ MeV, consistent with the $K^{*}(892)$ mass.
id cern-798021
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2004
record_format invenio
spelling cern-7980212023-08-03T04:00:03Zdoi:10.1016/j.physletb.2004.08.076http://cds.cern.ch/record/798021engLai, A.Marras, D.Bevan, A.Dosanjh, R.S.Gershon, T.J.Hay, B.Kalmus, G.E.Lazzeroni, C.Munday, D.J.Olaiya, E.Parker, Michael AndrewWhite, T.O.Wotton, S.A.Barr, G.Bocquet, G.Ceccucci, A.Cuhadar-Donszelmann, T.Cundy, D.D'Agostini, G.Doble, N.Falaleev, V.Gatignon, L.Gonidec, A.Gorini, B.Govi, G.Grafstrom, P.Kubischta, W.Lacourt, A.Norton, A.Palestini, S.Panzer-Steindel, B.Taureg, H.Velasco, M.Wahl, HeinrichCheshkov, C.Hristov, P.Kekelidze, V.Litov, L.Madigojine, D.Molokanova, N.Potrebenikov, Yu.Stoynev, S.Zinchenko, A.Knowles, I.Martin, V.Sacco, R.Walker, A.Contalbrigo, M.Dalpiaz, P.Duclos, J.Frabetti, P.L.Gianoli, A.Martini, M.Petrucci, F.Savrie, M.Bizzeti, A.Calvetti, M.Collazuol, G.Graziani, G.Iacopini, E.Lenti, M.Martelli, F.Veltri, M.Becker, H.G.Eppard, K.Eppard, M.Fox, H.Kalter, A.Kleinknecht, K.Koch, U.Kopke, L.Lopes da Silva, P.Marouelli, P.Pellmann, I.Peters, A.Renk, B.Schmidt, S.A.Schonharting, V.Schue, Y.Wanke, R.Winhart, A.Wittgen, M.Chollet, J.C.Fayard, L.Iconomidou-Fayard, L.Ocariz, J.Unal, G.Wingerter-Seez, I.Anzivino, G.Cenci, P.Imbergamo, E.Lubrano, P.Mestvirishvili, A.Nappi, A.Pepe, M.Piccini, M.Bertanza, L.Carosi, R.Casali, R.Cerri, C.Cirilli, M.Costantini, F.Fantechi, R.Giudici, S.Mannelli, I.Pierazzini, G.Sozzi, M.Cheze, J.B.Cogan, J.De Beer, M.Debu, P.Formica, A.Granier de Cassagnac, R.Mazzucato, E.Peyaud, B.Turlay, R.Vallage, B.Holder, M.Maier, A.Ziolkowski, M.Arcidiacono, R.Biino, C.Cartiglia, N.Marchetto, F.Menichetti, Ezio A.Pastrone, N.Nassalski, J.Rondio, E.Szleper, M.Wislicki, W.Wronka, S.Dibon, H.Fischer, G.Jeitler, M.Markytan, M.Mikulec, I.Neuhofer, G.Pernicka, M.Taurok, A.Widhalm, L.Measurement of $K_{e3}^{0}$ form factorsParticle Physics - ExperimentThe semi-leptonic decay of the neutral K meson $K^{0}_{L} \to \pi^{\pm}e^{\mp}\nu (K_{e3})$, was used to study the strangeness-changing weak interaction of hadrons. A sample of 5.6 million reconstructed events recorded by the NA48 experiment was used to measure the Dalitz plot density. Admitting all possible Lorentz-covariant couplings, the form factors for vector $(f_{+}(q^{2}))$, scalar $(f_{S})$ and tensor $(f_{T})$ interactions were measured. The linear slope of the vector form factor $\lambda_{+} = 0.0284 \pm 0.0007 \pm 0.0013$ and values for the ratios $|f_{S}/f_{+}(0)|=0.015^{+0.007}_{-0.010} \pm 0.012$ and $|f_{T}/f_{+}(0)|=0.05^{+0.03}_{-0.04} \pm 0.03$ were obtained. The values for $f_{S}$ and for $f_{T}$ are consistent with zero. Assuming only vector-axial vector couplings, $\lambda_{+} = 0.02888 \pm 0.0004 \pm 0.0011$ and a good fit consistent with pure V-A couplings were obtained. Alternatively a fit to a dipole form factor yields a pole mass of $M = 859 \pm 18$ MeV, consistent with the $K^{*}(892)$ mass.The semileptonic decay of the neutral K meson, KL0→π±e∓ν ( Ke3 ), was used to study the strangeness-changing weak interaction of hadrons. A sample of 5.6 million reconstructed events recorded by the NA48 experiment was used to measure the Dalitz plot density. Admitting all possible Lorentz-covariant couplings, the form factors for vector (f+(q2)) , scalar ( fS ) and tensor ( fT ) interactions were measured. The linear slope of the vector form factor λ+=0.0284±0.0007±0.0013 and values for the ratios |fS/f+(0)|=0.015−0.010+0.007±0.012 and |fT/f+(0)|=0.05−0.04+0.03±0.03 were obtained. The values for fS and fT are consistent with zero. Assuming only vector–axial-vector couplings, λ+=0.0288±0.0004±0.0011 and a good fit consistent with pure V–A couplings were obtained. Alternatively, a fit to a dipole form factor yields a pole mass of M=859±18 MeV , consistent with the K*(892) mass.The semileptonic decay of the neutral K meson, KL -> pi e nu (Ke3), was used to study the strangeness-changing weak interaction of hadrons. A sample of 5.6 million reconstructed events recorded by the NA48 experiment was used to measure the Dalitz plot density. Admitting all possible Lorentz-covariant couplings, the form factors for vector (f_+(q^2)), scalar (f_S) and tensor (f_T) interactions were measured. The linear slope of the vector form factor lambda_+ = 0.0284+-0.0007+-0.0013 and values for the ratios |f_S/f_+(0)| = 0.015^{+0.007}_{-0.010}+-0.012 and |f_T/f_+(0)| = 0.05^{+0.03}_{-0.04}+-0.03 were obtained. The values for f_S and f_T are consistent with zero. Assuming only Vector-Axial vector couplings, lambda_+ = 0.0288+-0.0004+-0.0011 and a good fit consistent with pure V-A couplings were obtained. Alternatively, a fit to a dipole form factor yields a pole mass of M = 859+-18 MeV, consistent with the K^*(892) mass.hep-ex/0410065CERN-PH-EP-2004-048CERN-PH-EP-2004-048oai:cds.cern.ch:7980212004-08-26
spellingShingle Particle Physics - Experiment
Lai, A.
Marras, D.
Bevan, A.
Dosanjh, R.S.
Gershon, T.J.
Hay, B.
Kalmus, G.E.
Lazzeroni, C.
Munday, D.J.
Olaiya, E.
Parker, Michael Andrew
White, T.O.
Wotton, S.A.
Barr, G.
Bocquet, G.
Ceccucci, A.
Cuhadar-Donszelmann, T.
Cundy, D.
D'Agostini, G.
Doble, N.
Falaleev, V.
Gatignon, L.
Gonidec, A.
Gorini, B.
Govi, G.
Grafstrom, P.
Kubischta, W.
Lacourt, A.
Norton, A.
Palestini, S.
Panzer-Steindel, B.
Taureg, H.
Velasco, M.
Wahl, Heinrich
Cheshkov, C.
Hristov, P.
Kekelidze, V.
Litov, L.
Madigojine, D.
Molokanova, N.
Potrebenikov, Yu.
Stoynev, S.
Zinchenko, A.
Knowles, I.
Martin, V.
Sacco, R.
Walker, A.
Contalbrigo, M.
Dalpiaz, P.
Duclos, J.
Frabetti, P.L.
Gianoli, A.
Martini, M.
Petrucci, F.
Savrie, M.
Bizzeti, A.
Calvetti, M.
Collazuol, G.
Graziani, G.
Iacopini, E.
Lenti, M.
Martelli, F.
Veltri, M.
Becker, H.G.
Eppard, K.
Eppard, M.
Fox, H.
Kalter, A.
Kleinknecht, K.
Koch, U.
Kopke, L.
Lopes da Silva, P.
Marouelli, P.
Pellmann, I.
Peters, A.
Renk, B.
Schmidt, S.A.
Schonharting, V.
Schue, Y.
Wanke, R.
Winhart, A.
Wittgen, M.
Chollet, J.C.
Fayard, L.
Iconomidou-Fayard, L.
Ocariz, J.
Unal, G.
Wingerter-Seez, I.
Anzivino, G.
Cenci, P.
Imbergamo, E.
Lubrano, P.
Mestvirishvili, A.
Nappi, A.
Pepe, M.
Piccini, M.
Bertanza, L.
Carosi, R.
Casali, R.
Cerri, C.
Cirilli, M.
Costantini, F.
Fantechi, R.
Giudici, S.
Mannelli, I.
Pierazzini, G.
Sozzi, M.
Cheze, J.B.
Cogan, J.
De Beer, M.
Debu, P.
Formica, A.
Granier de Cassagnac, R.
Mazzucato, E.
Peyaud, B.
Turlay, R.
Vallage, B.
Holder, M.
Maier, A.
Ziolkowski, M.
Arcidiacono, R.
Biino, C.
Cartiglia, N.
Marchetto, F.
Menichetti, Ezio A.
Pastrone, N.
Nassalski, J.
Rondio, E.
Szleper, M.
Wislicki, W.
Wronka, S.
Dibon, H.
Fischer, G.
Jeitler, M.
Markytan, M.
Mikulec, I.
Neuhofer, G.
Pernicka, M.
Taurok, A.
Widhalm, L.
Measurement of $K_{e3}^{0}$ form factors
title Measurement of $K_{e3}^{0}$ form factors
title_full Measurement of $K_{e3}^{0}$ form factors
title_fullStr Measurement of $K_{e3}^{0}$ form factors
title_full_unstemmed Measurement of $K_{e3}^{0}$ form factors
title_short Measurement of $K_{e3}^{0}$ form factors
title_sort measurement of $k_{e3}^{0}$ form factors
topic Particle Physics - Experiment
url https://dx.doi.org/10.1016/j.physletb.2004.08.076
http://cds.cern.ch/record/798021
work_keys_str_mv AT laia measurementofke30formfactors
AT marrasd measurementofke30formfactors
AT bevana measurementofke30formfactors
AT dosanjhrs measurementofke30formfactors
AT gershontj measurementofke30formfactors
AT hayb measurementofke30formfactors
AT kalmusge measurementofke30formfactors
AT lazzeronic measurementofke30formfactors
AT mundaydj measurementofke30formfactors
AT olaiyae measurementofke30formfactors
AT parkermichaelandrew measurementofke30formfactors
AT whiteto measurementofke30formfactors
AT wottonsa measurementofke30formfactors
AT barrg measurementofke30formfactors
AT bocquetg measurementofke30formfactors
AT ceccuccia measurementofke30formfactors
AT cuhadardonszelmannt measurementofke30formfactors
AT cundyd measurementofke30formfactors
AT dagostinig measurementofke30formfactors
AT doblen measurementofke30formfactors
AT falaleevv measurementofke30formfactors
AT gatignonl measurementofke30formfactors
AT gonideca measurementofke30formfactors
AT gorinib measurementofke30formfactors
AT govig measurementofke30formfactors
AT grafstromp measurementofke30formfactors
AT kubischtaw measurementofke30formfactors
AT lacourta measurementofke30formfactors
AT nortona measurementofke30formfactors
AT palestinis measurementofke30formfactors
AT panzersteindelb measurementofke30formfactors
AT tauregh measurementofke30formfactors
AT velascom measurementofke30formfactors
AT wahlheinrich measurementofke30formfactors
AT cheshkovc measurementofke30formfactors
AT hristovp measurementofke30formfactors
AT kekelidzev measurementofke30formfactors
AT litovl measurementofke30formfactors
AT madigojined measurementofke30formfactors
AT molokanovan measurementofke30formfactors
AT potrebenikovyu measurementofke30formfactors
AT stoynevs measurementofke30formfactors
AT zinchenkoa measurementofke30formfactors
AT knowlesi measurementofke30formfactors
AT martinv measurementofke30formfactors
AT saccor measurementofke30formfactors
AT walkera measurementofke30formfactors
AT contalbrigom measurementofke30formfactors
AT dalpiazp measurementofke30formfactors
AT duclosj measurementofke30formfactors
AT frabettipl measurementofke30formfactors
AT gianolia measurementofke30formfactors
AT martinim measurementofke30formfactors
AT petruccif measurementofke30formfactors
AT savriem measurementofke30formfactors
AT bizzetia measurementofke30formfactors
AT calvettim measurementofke30formfactors
AT collazuolg measurementofke30formfactors
AT grazianig measurementofke30formfactors
AT iacopinie measurementofke30formfactors
AT lentim measurementofke30formfactors
AT martellif measurementofke30formfactors
AT veltrim measurementofke30formfactors
AT beckerhg measurementofke30formfactors
AT eppardk measurementofke30formfactors
AT eppardm measurementofke30formfactors
AT foxh measurementofke30formfactors
AT kaltera measurementofke30formfactors
AT kleinknechtk measurementofke30formfactors
AT kochu measurementofke30formfactors
AT kopkel measurementofke30formfactors
AT lopesdasilvap measurementofke30formfactors
AT marouellip measurementofke30formfactors
AT pellmanni measurementofke30formfactors
AT petersa measurementofke30formfactors
AT renkb measurementofke30formfactors
AT schmidtsa measurementofke30formfactors
AT schonhartingv measurementofke30formfactors
AT schuey measurementofke30formfactors
AT wanker measurementofke30formfactors
AT winharta measurementofke30formfactors
AT wittgenm measurementofke30formfactors
AT cholletjc measurementofke30formfactors
AT fayardl measurementofke30formfactors
AT iconomidoufayardl measurementofke30formfactors
AT ocarizj measurementofke30formfactors
AT unalg measurementofke30formfactors
AT wingerterseezi measurementofke30formfactors
AT anzivinog measurementofke30formfactors
AT cencip measurementofke30formfactors
AT imbergamoe measurementofke30formfactors
AT lubranop measurementofke30formfactors
AT mestvirishvilia measurementofke30formfactors
AT nappia measurementofke30formfactors
AT pepem measurementofke30formfactors
AT piccinim measurementofke30formfactors
AT bertanzal measurementofke30formfactors
AT carosir measurementofke30formfactors
AT casalir measurementofke30formfactors
AT cerric measurementofke30formfactors
AT cirillim measurementofke30formfactors
AT costantinif measurementofke30formfactors
AT fantechir measurementofke30formfactors
AT giudicis measurementofke30formfactors
AT mannellii measurementofke30formfactors
AT pierazzinig measurementofke30formfactors
AT sozzim measurementofke30formfactors
AT chezejb measurementofke30formfactors
AT coganj measurementofke30formfactors
AT debeerm measurementofke30formfactors
AT debup measurementofke30formfactors
AT formicaa measurementofke30formfactors
AT granierdecassagnacr measurementofke30formfactors
AT mazzucatoe measurementofke30formfactors
AT peyaudb measurementofke30formfactors
AT turlayr measurementofke30formfactors
AT vallageb measurementofke30formfactors
AT holderm measurementofke30formfactors
AT maiera measurementofke30formfactors
AT ziolkowskim measurementofke30formfactors
AT arcidiaconor measurementofke30formfactors
AT biinoc measurementofke30formfactors
AT cartiglian measurementofke30formfactors
AT marchettof measurementofke30formfactors
AT menichettiezioa measurementofke30formfactors
AT pastronen measurementofke30formfactors
AT nassalskij measurementofke30formfactors
AT rondioe measurementofke30formfactors
AT szleperm measurementofke30formfactors
AT wislickiw measurementofke30formfactors
AT wronkas measurementofke30formfactors
AT dibonh measurementofke30formfactors
AT fischerg measurementofke30formfactors
AT jeitlerm measurementofke30formfactors
AT markytanm measurementofke30formfactors
AT mikuleci measurementofke30formfactors
AT neuhoferg measurementofke30formfactors
AT pernickam measurementofke30formfactors
AT tauroka measurementofke30formfactors
AT widhalml measurementofke30formfactors