Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra

Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberration...
Ausführliche Beschreibung

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Autor*in:	Sorzano, Carlos Oscar S [verfasserIn] Otero, Abraham Olmos, Estefanía M Carazo, José María

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2009

Schlagwörter:	Modulation Transfer Function Astigmatism Power Spectrum Density Spherical Aberration Average Sensitivity

Anmerkung:	© Sorzano et al; licensee BioMed Central Ltd. 2009

Übergeordnetes Werk:	Enthalten in: BMC structural biology - London : BioMed Central, 2001, 9(2009), 1 vom: 26. März
Übergeordnetes Werk:	volume:9 ; year:2009 ; number:1 ; day:26 ; month:03

Links:	Volltext

DOI / URN:	10.1186/1472-6807-9-18

Katalog-ID:	SPR028605683

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520			\|a Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here.
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650		4	\|a Astigmatism \|7 (dpeaa)DE-He213
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650		4	\|a Spherical Aberration \|7 (dpeaa)DE-He213
650		4	\|a Average Sensitivity \|7 (dpeaa)DE-He213
700	1		\|a Otero, Abraham \|4 aut
700	1		\|a Olmos, Estefanía M \|4 aut
700	1		\|a Carazo, José María \|4 aut
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allfields	10.1186/1472-6807-9-18 doi (DE-627)SPR028605683 (SPR)1472-6807-9-18-e DE-627 ger DE-627 rakwb eng Sorzano, Carlos Oscar S verfasserin aut Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Sorzano et al; licensee BioMed Central Ltd. 2009 Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. Modulation Transfer Function (dpeaa)DE-He213 Astigmatism (dpeaa)DE-He213 Power Spectrum Density (dpeaa)DE-He213 Spherical Aberration (dpeaa)DE-He213 Average Sensitivity (dpeaa)DE-He213 Otero, Abraham aut Olmos, Estefanía M aut Carazo, José María aut Enthalten in BMC structural biology London : BioMed Central, 2001 9(2009), 1 vom: 26. März (DE-627)331018810 (DE-600)2050440-8 1472-6807 nnns volume:9 year:2009 number:1 day:26 month:03 https://dx.doi.org/10.1186/1472-6807-9-18 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2009 1 26 03
spelling	10.1186/1472-6807-9-18 doi (DE-627)SPR028605683 (SPR)1472-6807-9-18-e DE-627 ger DE-627 rakwb eng Sorzano, Carlos Oscar S verfasserin aut Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Sorzano et al; licensee BioMed Central Ltd. 2009 Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. Modulation Transfer Function (dpeaa)DE-He213 Astigmatism (dpeaa)DE-He213 Power Spectrum Density (dpeaa)DE-He213 Spherical Aberration (dpeaa)DE-He213 Average Sensitivity (dpeaa)DE-He213 Otero, Abraham aut Olmos, Estefanía M aut Carazo, José María aut Enthalten in BMC structural biology London : BioMed Central, 2001 9(2009), 1 vom: 26. März (DE-627)331018810 (DE-600)2050440-8 1472-6807 nnns volume:9 year:2009 number:1 day:26 month:03 https://dx.doi.org/10.1186/1472-6807-9-18 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2009 1 26 03
allfields_unstemmed	10.1186/1472-6807-9-18 doi (DE-627)SPR028605683 (SPR)1472-6807-9-18-e DE-627 ger DE-627 rakwb eng Sorzano, Carlos Oscar S verfasserin aut Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Sorzano et al; licensee BioMed Central Ltd. 2009 Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. Modulation Transfer Function (dpeaa)DE-He213 Astigmatism (dpeaa)DE-He213 Power Spectrum Density (dpeaa)DE-He213 Spherical Aberration (dpeaa)DE-He213 Average Sensitivity (dpeaa)DE-He213 Otero, Abraham aut Olmos, Estefanía M aut Carazo, José María aut Enthalten in BMC structural biology London : BioMed Central, 2001 9(2009), 1 vom: 26. März (DE-627)331018810 (DE-600)2050440-8 1472-6807 nnns volume:9 year:2009 number:1 day:26 month:03 https://dx.doi.org/10.1186/1472-6807-9-18 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2009 1 26 03
allfieldsGer	10.1186/1472-6807-9-18 doi (DE-627)SPR028605683 (SPR)1472-6807-9-18-e DE-627 ger DE-627 rakwb eng Sorzano, Carlos Oscar S verfasserin aut Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Sorzano et al; licensee BioMed Central Ltd. 2009 Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. Modulation Transfer Function (dpeaa)DE-He213 Astigmatism (dpeaa)DE-He213 Power Spectrum Density (dpeaa)DE-He213 Spherical Aberration (dpeaa)DE-He213 Average Sensitivity (dpeaa)DE-He213 Otero, Abraham aut Olmos, Estefanía M aut Carazo, José María aut Enthalten in BMC structural biology London : BioMed Central, 2001 9(2009), 1 vom: 26. März (DE-627)331018810 (DE-600)2050440-8 1472-6807 nnns volume:9 year:2009 number:1 day:26 month:03 https://dx.doi.org/10.1186/1472-6807-9-18 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2009 1 26 03
allfieldsSound	10.1186/1472-6807-9-18 doi (DE-627)SPR028605683 (SPR)1472-6807-9-18-e DE-627 ger DE-627 rakwb eng Sorzano, Carlos Oscar S verfasserin aut Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Sorzano et al; licensee BioMed Central Ltd. 2009 Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. Modulation Transfer Function (dpeaa)DE-He213 Astigmatism (dpeaa)DE-He213 Power Spectrum Density (dpeaa)DE-He213 Spherical Aberration (dpeaa)DE-He213 Average Sensitivity (dpeaa)DE-He213 Otero, Abraham aut Olmos, Estefanía M aut Carazo, José María aut Enthalten in BMC structural biology London : BioMed Central, 2001 9(2009), 1 vom: 26. März (DE-627)331018810 (DE-600)2050440-8 1472-6807 nnns volume:9 year:2009 number:1 day:26 month:03 https://dx.doi.org/10.1186/1472-6807-9-18 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 9 2009 1 26 03
language	English
source	Enthalten in BMC structural biology 9(2009), 1 vom: 26. März volume:9 year:2009 number:1 day:26 month:03
sourceStr	Enthalten in BMC structural biology 9(2009), 1 vom: 26. März volume:9 year:2009 number:1 day:26 month:03
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Modulation Transfer Function Astigmatism Power Spectrum Density Spherical Aberration Average Sensitivity
isfreeaccess_bool	true
container_title	BMC structural biology
authorswithroles_txt_mv	Sorzano, Carlos Oscar S @@aut@@ Otero, Abraham @@aut@@ Olmos, Estefanía M @@aut@@ Carazo, José María @@aut@@
publishDateDaySort_date	2009-03-26T00:00:00Z
hierarchy_top_id	331018810
id	SPR028605683
language_de	englisch
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author	Sorzano, Carlos Oscar S
spellingShingle	Sorzano, Carlos Oscar S misc Modulation Transfer Function misc Astigmatism misc Power Spectrum Density misc Spherical Aberration misc Average Sensitivity Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra
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topic_title	Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra Modulation Transfer Function (dpeaa)DE-He213 Astigmatism (dpeaa)DE-He213 Power Spectrum Density (dpeaa)DE-He213 Spherical Aberration (dpeaa)DE-He213 Average Sensitivity (dpeaa)DE-He213
topic	misc Modulation Transfer Function misc Astigmatism misc Power Spectrum Density misc Spherical Aberration misc Average Sensitivity
topic_unstemmed	misc Modulation Transfer Function misc Astigmatism misc Power Spectrum Density misc Spherical Aberration misc Average Sensitivity
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title	Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra
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title_full	Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra
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title_sort	error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power spectra
title_auth	Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra
abstract	Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. © Sorzano et al; licensee BioMed Central Ltd. 2009
abstractGer	Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. © Sorzano et al; licensee BioMed Central Ltd. 2009
abstract_unstemmed	Background The transmission electron microscope is used to acquire structural information of macromolecular complexes. However, as any other imaging device, it introduces optical aberrations that must be corrected if high-resolution structural information is to be obtained. The set of all aberrations are usually modeled in Fourier space by the so-called Contrast Transfer Function (CTF). Before correcting for the CTF, we must first estimate it from the electron micrographs. This is usually done by estimating a number of parameters specifying a theoretical model of the CTF. This estimation is performed by minimizing some error measure between the theoretical Power Spectrum Density (PSD) and the experimentally observed PSD. The high noise present in the micrographs, the possible local minima of the error function for estimating the CTF parameters, and the cross-talking between CTF parameters may cause errors in the estimated CTF parameters. Results In this paper, we explore the effect of these estimation errors on the theoretical CTF. For the CTF model proposed in [1] we show which are the most sensitive CTF parameters as well as the most sensitive background parameters. Moreover, we provide a methodology to reveal the internal structure of the CTF model (which parameters influence in which parameters) and to estimate the accuracy of each model parameter. Finally, we explore the effect of the variability in the detection of the CTF for CTF phase and amplitude correction. Conclusion We show that the estimation errors for the CTF detection methodology proposed in [1] does not show a significant deterioration of the CTF correction capabilities of subsequent algorithms. All together, the methodology described in this paper constitutes a powerful tool for the quantitative analysis of CTF models that can be applied to other models different from the one analyzed here. © Sorzano et al; licensee BioMed Central Ltd. 2009
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title_short	Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra
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Error analysis in the determination of the electron microscopical contrast transfer function parameters from experimental power Spectra

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