Visualizing the Invisible :: Imaging Techniques for the Structural Biologist.
Knowledge of the microscopic structure of biological systems is the key to understanding their physiological properties. Most of what we now know about this subject has been generated by techniques that produce images of the materials of interest, one way or another, and there is every reason to bel...
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| Format: | Elektronisch E-Book |
| Sprache: | English |
| Veröffentlicht: |
Oxford :
Oxford University Press, USA,
2012.
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| Schlagworte: | |
| Online-Zugang: | Volltext |
| Zusammenfassung: | Knowledge of the microscopic structure of biological systems is the key to understanding their physiological properties. Most of what we now know about this subject has been generated by techniques that produce images of the materials of interest, one way or another, and there is every reason to believe that the impact of these techniques on the biological sciences will be every bit as important in the future as they are today. Thus the 21st century biologist needs to understand how microscopic imaging techniques work, as it is likely that sooner or later he or she will have to use one or anot. |
| Beschreibung: | 1 online resource (397 pages) |
| Bibliographie: | Includes bibliographical references and index. |
| ISBN: | 9780199930722 0199930724 0199767092 9780199767090 1280595701 9781280595707 0190267844 9780190267841 9786613625533 6613625531 |
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| 100 | 1 | |a Moore, Peter. | |
| 245 | 1 | 0 | |a Visualizing the Invisible : |b Imaging Techniques for the Structural Biologist. |
| 260 | |a Oxford : |b Oxford University Press, USA, |c 2012. | ||
| 300 | |a 1 online resource (397 pages) | ||
| 336 | |a text |b txt |2 rdacontent | ||
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| 505 | 0 | |a Cover; Contents; Preface; Notes for the Reader; PART ONE: Fundamentals; 1. On the Scattering of Electromagnetic Radiation by Atoms andMolecules; 1.1 What is electromagnetic radiation?; 1.2 Atoms are electrically polarized by electromagnetic radiation; 1.3 Oscillating dipoles emit electromagnetic radiation; 1.4 The electrons in atoms and molecules scatter X-rays as though they were unbound; 1.5 The scattering of X-rays by molecules depends on atomic positions; 1.6 Radiation detectors measure energy, not field strength. | |
| 505 | 8 | |a 1.7 If the radiation being scattered is unpolarized, the polarization correction depends only on scattering angle1.8 The coherence length of the radiation used in scattered experiments affects the accuracy with which I[sub(d)] can be measured; 1.9 Measurement accuracy also depends on transverse coherence length; Problems; Appendix 1.1 Exponential notation, complex numbers, and Argand diagrams; Appendix 1.2 The polarization correction for unpolarized radiation; 2. Molecular Scattering and Fourier Transforms; 2.1 F(S) is a function of three angular variables. | |
| 505 | 8 | |a 2.2 Fourier series are a useful way to represent structures2.3 In the limit of d = 8, the Fourier series becomes the Fourier transformation; 2.4 The Great Experiment; 2.5 The shift theorem leads to a simple expression for the scattering of molecules; 2.6 The scaling theorem: Big things in real space are small things in reciprocal space; 2.7 The square wave and the Dirac delta function; 2.8 Multiplication in real and reciprocal space: The convolution theorem; 2.9 Instrument transfer functions and convolutions; 2.10 The autocorrelation theorem; 2.11 Rayleigh's theorem; Problems. | |
| 505 | 8 | |a 3. Scattering by Condensed Phases3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it; 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample; 3.3 Phase changes are indistinguishable from velocity changes; 3.4 Polarizabilities do not have to be real numbers; 3.5 Atomic polarization effects are small; 3.6 The frequency dependence of polarizabilities can be addressed classically; 3.7 When the imaginary part of a is large, energy is absorbed. | |
| 505 | 8 | |a 3.8 The refractive index of substances for X-rays is less than 1.03.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different; 3.10 On the frequency dependence of atomic scattering factors for X-rays; 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts; 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients; 3.13 Scattering can be described using scattering lengths and cross sections; 3.14 Neutron scattering can be used to study molecular structure. | |
| 520 | |a Knowledge of the microscopic structure of biological systems is the key to understanding their physiological properties. Most of what we now know about this subject has been generated by techniques that produce images of the materials of interest, one way or another, and there is every reason to believe that the impact of these techniques on the biological sciences will be every bit as important in the future as they are today. Thus the 21st century biologist needs to understand how microscopic imaging techniques work, as it is likely that sooner or later he or she will have to use one or anot. | ||
| 504 | |a Includes bibliographical references and index. | ||
| 546 | |a English. | ||
| 650 | 0 | |a Ultrastructure (Biology) |0 http://id.loc.gov/authorities/subjects/sh85139504 | |
| 650 | 0 | |a Molecular structure. |0 http://id.loc.gov/authorities/subjects/sh85086594 | |
| 650 | 0 | |a Fourier transformations. |0 http://id.loc.gov/authorities/subjects/sh85051094 | |
| 650 | 0 | |a Imaging systems in biology. |0 http://id.loc.gov/authorities/subjects/sh87004825 | |
| 650 | 0 | |a Cytology |x Experiments. | |
| 650 | 0 | |a Molecular biology |x Experiments. | |
| 650 | 0 | |a Biology |x Experiments. |0 http://id.loc.gov/authorities/subjects/sh85014207 | |
| 650 | 2 | |a Molecular Structure |0 https://id.nlm.nih.gov/mesh/D015394 | |
| 650 | 6 | |a Ultrastructure (Biologie) | |
| 650 | 6 | |a Structure moléculaire. | |
| 650 | 6 | |a Imagerie en biologie. | |
| 650 | 6 | |a Cytologie |x Expériences. | |
| 650 | 6 | |a Biologie moléculaire |x Expériences. | |
| 650 | 6 | |a Biologie |x Expériences. | |
| 650 | 7 | |a ultrastructure. |2 aat | |
| 650 | 7 | |a molecular structure. |2 aat | |
| 650 | 7 | |a SCIENCE |x Life Sciences |x Cell Biology. |2 bisacsh | |
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| 650 | 7 | |a Imaging systems in biology |2 fast | |
| 650 | 7 | |a Molecular biology |x Experiments |2 fast | |
| 650 | 7 | |a Molecular structure |2 fast | |
| 650 | 7 | |a Ultrastructure (Biology) |2 fast | |
| 758 | |i has work: |a Visualizing the invisible (Text) |1 https://id.oclc.org/worldcat/entity/E39PCGjPvDHfby9xWvTf8HdkH3 |4 https://id.oclc.org/worldcat/ontology/hasWork | ||
| 776 | 0 | 8 | |i Print version: |a Moore, Peter, 1939- |t Visualizing the invisible. |d Oxford ; New York : Oxford University Press, ©2012 |z 9780199767090 |w (DLC) 2011027000 |w (OCoLC)744297062 |
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| 880 | 8 | |6 505-00/(S |a 3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it -- 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample -- 3.3 Phase changes are indistinguishable from velocity changes -- 3.4 Polarizabilities do not have to be real numbers -- 3.5 Atomic polarization effects are small -- 3.6 The frequency dependence of polarizabilities can be addressed classically -- 3.7 When the imaginary part of α is large, energy is absorbed -- 3.8 The refractive index of substances for X-rays is less than 1.0 -- 3.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different -- 3.10 On the frequency dependence of atomic scattering factors for X-rays -- 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts -- 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients -- 3.13 Scattering can be described using scattering lengths and cross sections -- 3.14 Neutron scattering can be used to study molecular structure -- 3.15 Electrons are strongly scattered by atoms and molecules -- 3.16 Electrons are scattered inelastically by atoms -- Problems -- Appendix 3.1 Forward scatter from a thin slab -- Appendix 3.2 A classical model for the motion of electrons in the presence of electromagnetic radiation -- Appendix 3.3 Energy absorption and the imaginary part of α -- PART TWO: Crystallography -- 4. On the Diffraction of X-rays by Crystals -- 4.1 The Fourier transform of a row of delta functions is a row of delta functions -- 4.2 Sampling in reciprocal space corresponds to replication in real space (and vice versa) -- 4.3 Crystals can be described as convolutions of molecules with lattices -- 4.4 Lattices "amplify" Fourier transforms. | |
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Datensatz im Suchindex
| DE-BY-FWS_katkey | ZDB-4-EBA-ocn793996708 |
|---|---|
| _version_ | 1816881795050766336 |
| adam_text | |
| any_adam_object | |
| author | Moore, Peter |
| author_facet | Moore, Peter |
| author_role | |
| author_sort | Moore, Peter |
| author_variant | p m pm |
| building | Verbundindex |
| bvnumber | localFWS |
| callnumber-first | Q - Science |
| callnumber-label | QH324 |
| callnumber-raw | QH324 .M66 2012 |
| callnumber-search | QH324 .M66 2012 |
| callnumber-sort | QH 3324 M66 42012 |
| callnumber-subject | QH - Natural History and Biology |
| collection | ZDB-4-EBA |
| contents | Cover; Contents; Preface; Notes for the Reader; PART ONE: Fundamentals; 1. On the Scattering of Electromagnetic Radiation by Atoms andMolecules; 1.1 What is electromagnetic radiation?; 1.2 Atoms are electrically polarized by electromagnetic radiation; 1.3 Oscillating dipoles emit electromagnetic radiation; 1.4 The electrons in atoms and molecules scatter X-rays as though they were unbound; 1.5 The scattering of X-rays by molecules depends on atomic positions; 1.6 Radiation detectors measure energy, not field strength. 1.7 If the radiation being scattered is unpolarized, the polarization correction depends only on scattering angle1.8 The coherence length of the radiation used in scattered experiments affects the accuracy with which I[sub(d)] can be measured; 1.9 Measurement accuracy also depends on transverse coherence length; Problems; Appendix 1.1 Exponential notation, complex numbers, and Argand diagrams; Appendix 1.2 The polarization correction for unpolarized radiation; 2. Molecular Scattering and Fourier Transforms; 2.1 F(S) is a function of three angular variables. 2.2 Fourier series are a useful way to represent structures2.3 In the limit of d = 8, the Fourier series becomes the Fourier transformation; 2.4 The Great Experiment; 2.5 The shift theorem leads to a simple expression for the scattering of molecules; 2.6 The scaling theorem: Big things in real space are small things in reciprocal space; 2.7 The square wave and the Dirac delta function; 2.8 Multiplication in real and reciprocal space: The convolution theorem; 2.9 Instrument transfer functions and convolutions; 2.10 The autocorrelation theorem; 2.11 Rayleigh's theorem; Problems. 3. Scattering by Condensed Phases3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it; 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample; 3.3 Phase changes are indistinguishable from velocity changes; 3.4 Polarizabilities do not have to be real numbers; 3.5 Atomic polarization effects are small; 3.6 The frequency dependence of polarizabilities can be addressed classically; 3.7 When the imaginary part of a is large, energy is absorbed. 3.8 The refractive index of substances for X-rays is less than 1.03.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different; 3.10 On the frequency dependence of atomic scattering factors for X-rays; 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts; 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients; 3.13 Scattering can be described using scattering lengths and cross sections; 3.14 Neutron scattering can be used to study molecular structure. |
| ctrlnum | (OCoLC)793996708 |
| dewey-full | 571.6 571.633 |
| dewey-hundreds | 500 - Natural sciences and mathematics |
| dewey-ones | 571 - Physiology & related subjects |
| dewey-raw | 571.6 571.633 |
| dewey-search | 571.6 571.633 |
| dewey-sort | 3571.6 |
| dewey-tens | 570 - Biology |
| discipline | Biologie |
| format | Electronic eBook |
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On the Scattering of Electromagnetic Radiation by Atoms andMolecules; 1.1 What is electromagnetic radiation?; 1.2 Atoms are electrically polarized by electromagnetic radiation; 1.3 Oscillating dipoles emit electromagnetic radiation; 1.4 The electrons in atoms and molecules scatter X-rays as though they were unbound; 1.5 The scattering of X-rays by molecules depends on atomic positions; 1.6 Radiation detectors measure energy, not field strength.</subfield></datafield><datafield tag="505" ind1="8" ind2=" "><subfield code="a">1.7 If the radiation being scattered is unpolarized, the polarization correction depends only on scattering angle1.8 The coherence length of the radiation used in scattered experiments affects the accuracy with which I[sub(d)] can be measured; 1.9 Measurement accuracy also depends on transverse coherence length; Problems; Appendix 1.1 Exponential notation, complex numbers, and Argand diagrams; Appendix 1.2 The polarization correction for unpolarized radiation; 2. 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Scattering by Condensed Phases3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it; 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample; 3.3 Phase changes are indistinguishable from velocity changes; 3.4 Polarizabilities do not have to be real numbers; 3.5 Atomic polarization effects are small; 3.6 The frequency dependence of polarizabilities can be addressed classically; 3.7 When the imaginary part of a is large, energy is absorbed.</subfield></datafield><datafield tag="505" ind1="8" ind2=" "><subfield code="a">3.8 The refractive index of substances for X-rays is less than 1.03.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different; 3.10 On the frequency dependence of atomic scattering factors for X-rays; 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts; 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients; 3.13 Scattering can be described using scattering lengths and cross sections; 3.14 Neutron scattering can be used to study molecular structure.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Knowledge of the microscopic structure of biological systems is the key to understanding their physiological properties. Most of what we now know about this subject has been generated by techniques that produce images of the materials of interest, one way or another, and there is every reason to believe that the impact of these techniques on the biological sciences will be every bit as important in the future as they are today. 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New York : Oxford University Press, ©2012</subfield><subfield code="z">9780199767090</subfield><subfield code="w">(DLC) 2011027000</subfield><subfield code="w">(OCoLC)744297062</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="l">FWS01</subfield><subfield code="p">ZDB-4-EBA</subfield><subfield code="q">FWS_PDA_EBA</subfield><subfield code="u">https://search.ebscohost.com/login.aspx?direct=true&scope=site&db=nlebk&AN=454382</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="880" ind1="8" ind2=" "><subfield code="6">505-00/(S</subfield><subfield code="a">3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it -- 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample -- 3.3 Phase changes are indistinguishable from velocity changes -- 3.4 Polarizabilities do not have to be real numbers -- 3.5 Atomic polarization effects are small -- 3.6 The frequency dependence of polarizabilities can be addressed classically -- 3.7 When the imaginary part of α is large, energy is absorbed -- 3.8 The refractive index of substances for X-rays is less than 1.0 -- 3.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different -- 3.10 On the frequency dependence of atomic scattering factors for X-rays -- 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts -- 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients -- 3.13 Scattering can be described using scattering lengths and cross sections -- 3.14 Neutron scattering can be used to study molecular structure -- 3.15 Electrons are strongly scattered by atoms and molecules -- 3.16 Electrons are scattered inelastically by atoms -- Problems -- Appendix 3.1 Forward scatter from a thin slab -- Appendix 3.2 A classical model for the motion of electrons in the presence of electromagnetic radiation -- Appendix 3.3 Energy absorption and the imaginary part of α -- PART TWO: Crystallography -- 4. 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| id | ZDB-4-EBA-ocn793996708 |
| illustrated | Not Illustrated |
| indexdate | 2024-11-27T13:18:23Z |
| institution | BVB |
| isbn | 9780199930722 0199930724 0199767092 9780199767090 1280595701 9781280595707 0190267844 9780190267841 9786613625533 6613625531 |
| language | English |
| oclc_num | 793996708 |
| open_access_boolean | |
| owner | MAIN DE-863 DE-BY-FWS |
| owner_facet | MAIN DE-863 DE-BY-FWS |
| physical | 1 online resource (397 pages) |
| psigel | ZDB-4-EBA |
| publishDate | 2012 |
| publishDateSearch | 2012 |
| publishDateSort | 2012 |
| publisher | Oxford University Press, USA, |
| record_format | marc |
| spelling | Moore, Peter. Visualizing the Invisible : Imaging Techniques for the Structural Biologist. Oxford : Oxford University Press, USA, 2012. 1 online resource (397 pages) text txt rdacontent computer c rdamedia online resource cr rdacarrier data file rda Print version record. Cover; Contents; Preface; Notes for the Reader; PART ONE: Fundamentals; 1. On the Scattering of Electromagnetic Radiation by Atoms andMolecules; 1.1 What is electromagnetic radiation?; 1.2 Atoms are electrically polarized by electromagnetic radiation; 1.3 Oscillating dipoles emit electromagnetic radiation; 1.4 The electrons in atoms and molecules scatter X-rays as though they were unbound; 1.5 The scattering of X-rays by molecules depends on atomic positions; 1.6 Radiation detectors measure energy, not field strength. 1.7 If the radiation being scattered is unpolarized, the polarization correction depends only on scattering angle1.8 The coherence length of the radiation used in scattered experiments affects the accuracy with which I[sub(d)] can be measured; 1.9 Measurement accuracy also depends on transverse coherence length; Problems; Appendix 1.1 Exponential notation, complex numbers, and Argand diagrams; Appendix 1.2 The polarization correction for unpolarized radiation; 2. Molecular Scattering and Fourier Transforms; 2.1 F(S) is a function of three angular variables. 2.2 Fourier series are a useful way to represent structures2.3 In the limit of d = 8, the Fourier series becomes the Fourier transformation; 2.4 The Great Experiment; 2.5 The shift theorem leads to a simple expression for the scattering of molecules; 2.6 The scaling theorem: Big things in real space are small things in reciprocal space; 2.7 The square wave and the Dirac delta function; 2.8 Multiplication in real and reciprocal space: The convolution theorem; 2.9 Instrument transfer functions and convolutions; 2.10 The autocorrelation theorem; 2.11 Rayleigh's theorem; Problems. 3. Scattering by Condensed Phases3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it; 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample; 3.3 Phase changes are indistinguishable from velocity changes; 3.4 Polarizabilities do not have to be real numbers; 3.5 Atomic polarization effects are small; 3.6 The frequency dependence of polarizabilities can be addressed classically; 3.7 When the imaginary part of a is large, energy is absorbed. 3.8 The refractive index of substances for X-rays is less than 1.03.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different; 3.10 On the frequency dependence of atomic scattering factors for X-rays; 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts; 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients; 3.13 Scattering can be described using scattering lengths and cross sections; 3.14 Neutron scattering can be used to study molecular structure. Knowledge of the microscopic structure of biological systems is the key to understanding their physiological properties. Most of what we now know about this subject has been generated by techniques that produce images of the materials of interest, one way or another, and there is every reason to believe that the impact of these techniques on the biological sciences will be every bit as important in the future as they are today. Thus the 21st century biologist needs to understand how microscopic imaging techniques work, as it is likely that sooner or later he or she will have to use one or anot. Includes bibliographical references and index. English. Ultrastructure (Biology) http://id.loc.gov/authorities/subjects/sh85139504 Molecular structure. http://id.loc.gov/authorities/subjects/sh85086594 Fourier transformations. http://id.loc.gov/authorities/subjects/sh85051094 Imaging systems in biology. http://id.loc.gov/authorities/subjects/sh87004825 Cytology Experiments. Molecular biology Experiments. Biology Experiments. http://id.loc.gov/authorities/subjects/sh85014207 Molecular Structure https://id.nlm.nih.gov/mesh/D015394 Ultrastructure (Biologie) Structure moléculaire. Imagerie en biologie. Cytologie Expériences. Biologie moléculaire Expériences. Biologie Expériences. ultrastructure. aat molecular structure. aat SCIENCE Life Sciences Cell Biology. bisacsh Biology Experiments fast Cytology Experiments fast Fourier transformations fast Imaging systems in biology fast Molecular biology Experiments fast Molecular structure fast Ultrastructure (Biology) fast has work: Visualizing the invisible (Text) https://id.oclc.org/worldcat/entity/E39PCGjPvDHfby9xWvTf8HdkH3 https://id.oclc.org/worldcat/ontology/hasWork Print version: Moore, Peter, 1939- Visualizing the invisible. Oxford ; New York : Oxford University Press, ©2012 9780199767090 (DLC) 2011027000 (OCoLC)744297062 FWS01 ZDB-4-EBA FWS_PDA_EBA https://search.ebscohost.com/login.aspx?direct=true&scope=site&db=nlebk&AN=454382 Volltext 505-00/(S 3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it -- 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample -- 3.3 Phase changes are indistinguishable from velocity changes -- 3.4 Polarizabilities do not have to be real numbers -- 3.5 Atomic polarization effects are small -- 3.6 The frequency dependence of polarizabilities can be addressed classically -- 3.7 When the imaginary part of α is large, energy is absorbed -- 3.8 The refractive index of substances for X-rays is less than 1.0 -- 3.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different -- 3.10 On the frequency dependence of atomic scattering factors for X-rays -- 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts -- 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients -- 3.13 Scattering can be described using scattering lengths and cross sections -- 3.14 Neutron scattering can be used to study molecular structure -- 3.15 Electrons are strongly scattered by atoms and molecules -- 3.16 Electrons are scattered inelastically by atoms -- Problems -- Appendix 3.1 Forward scatter from a thin slab -- Appendix 3.2 A classical model for the motion of electrons in the presence of electromagnetic radiation -- Appendix 3.3 Energy absorption and the imaginary part of α -- PART TWO: Crystallography -- 4. On the Diffraction of X-rays by Crystals -- 4.1 The Fourier transform of a row of delta functions is a row of delta functions -- 4.2 Sampling in reciprocal space corresponds to replication in real space (and vice versa) -- 4.3 Crystals can be described as convolutions of molecules with lattices -- 4.4 Lattices "amplify" Fourier transforms. |
| spellingShingle | Moore, Peter Visualizing the Invisible : Imaging Techniques for the Structural Biologist. Cover; Contents; Preface; Notes for the Reader; PART ONE: Fundamentals; 1. On the Scattering of Electromagnetic Radiation by Atoms andMolecules; 1.1 What is electromagnetic radiation?; 1.2 Atoms are electrically polarized by electromagnetic radiation; 1.3 Oscillating dipoles emit electromagnetic radiation; 1.4 The electrons in atoms and molecules scatter X-rays as though they were unbound; 1.5 The scattering of X-rays by molecules depends on atomic positions; 1.6 Radiation detectors measure energy, not field strength. 1.7 If the radiation being scattered is unpolarized, the polarization correction depends only on scattering angle1.8 The coherence length of the radiation used in scattered experiments affects the accuracy with which I[sub(d)] can be measured; 1.9 Measurement accuracy also depends on transverse coherence length; Problems; Appendix 1.1 Exponential notation, complex numbers, and Argand diagrams; Appendix 1.2 The polarization correction for unpolarized radiation; 2. Molecular Scattering and Fourier Transforms; 2.1 F(S) is a function of three angular variables. 2.2 Fourier series are a useful way to represent structures2.3 In the limit of d = 8, the Fourier series becomes the Fourier transformation; 2.4 The Great Experiment; 2.5 The shift theorem leads to a simple expression for the scattering of molecules; 2.6 The scaling theorem: Big things in real space are small things in reciprocal space; 2.7 The square wave and the Dirac delta function; 2.8 Multiplication in real and reciprocal space: The convolution theorem; 2.9 Instrument transfer functions and convolutions; 2.10 The autocorrelation theorem; 2.11 Rayleigh's theorem; Problems. 3. Scattering by Condensed Phases3.1 The forward scatter from macroscopic samples is 90° out of phase with respect to the radiation that induces it; 3.2 Scattering alters the phase of all the radiation that passes through a transparent sample; 3.3 Phase changes are indistinguishable from velocity changes; 3.4 Polarizabilities do not have to be real numbers; 3.5 Atomic polarization effects are small; 3.6 The frequency dependence of polarizabilities can be addressed classically; 3.7 When the imaginary part of a is large, energy is absorbed. 3.8 The refractive index of substances for X-rays is less than 1.03.9 The wavelength dependences of the processes that control light and X-ray polarizabilities are different; 3.10 On the frequency dependence of atomic scattering factors for X-rays; 3.11 Real X-ray absorption and dispersion spectra do not look the way classical theory predicts; 3.12 The imaginary component of f can be determined by measuring mass absorption coefficients; 3.13 Scattering can be described using scattering lengths and cross sections; 3.14 Neutron scattering can be used to study molecular structure. Ultrastructure (Biology) http://id.loc.gov/authorities/subjects/sh85139504 Molecular structure. http://id.loc.gov/authorities/subjects/sh85086594 Fourier transformations. http://id.loc.gov/authorities/subjects/sh85051094 Imaging systems in biology. http://id.loc.gov/authorities/subjects/sh87004825 Cytology Experiments. Molecular biology Experiments. Biology Experiments. http://id.loc.gov/authorities/subjects/sh85014207 Molecular Structure https://id.nlm.nih.gov/mesh/D015394 Ultrastructure (Biologie) Structure moléculaire. Imagerie en biologie. Cytologie Expériences. Biologie moléculaire Expériences. Biologie Expériences. ultrastructure. aat molecular structure. aat SCIENCE Life Sciences Cell Biology. bisacsh Biology Experiments fast Cytology Experiments fast Fourier transformations fast Imaging systems in biology fast Molecular biology Experiments fast Molecular structure fast Ultrastructure (Biology) fast |
| subject_GND | http://id.loc.gov/authorities/subjects/sh85139504 http://id.loc.gov/authorities/subjects/sh85086594 http://id.loc.gov/authorities/subjects/sh85051094 http://id.loc.gov/authorities/subjects/sh87004825 http://id.loc.gov/authorities/subjects/sh85014207 https://id.nlm.nih.gov/mesh/D015394 |
| title | Visualizing the Invisible : Imaging Techniques for the Structural Biologist. |
| title_auth | Visualizing the Invisible : Imaging Techniques for the Structural Biologist. |
| title_exact_search | Visualizing the Invisible : Imaging Techniques for the Structural Biologist. |
| title_full | Visualizing the Invisible : Imaging Techniques for the Structural Biologist. |
| title_fullStr | Visualizing the Invisible : Imaging Techniques for the Structural Biologist. |
| title_full_unstemmed | Visualizing the Invisible : Imaging Techniques for the Structural Biologist. |
| title_short | Visualizing the Invisible : |
| title_sort | visualizing the invisible imaging techniques for the structural biologist |
| title_sub | Imaging Techniques for the Structural Biologist. |
| topic | Ultrastructure (Biology) http://id.loc.gov/authorities/subjects/sh85139504 Molecular structure. http://id.loc.gov/authorities/subjects/sh85086594 Fourier transformations. http://id.loc.gov/authorities/subjects/sh85051094 Imaging systems in biology. http://id.loc.gov/authorities/subjects/sh87004825 Cytology Experiments. Molecular biology Experiments. Biology Experiments. http://id.loc.gov/authorities/subjects/sh85014207 Molecular Structure https://id.nlm.nih.gov/mesh/D015394 Ultrastructure (Biologie) Structure moléculaire. Imagerie en biologie. Cytologie Expériences. Biologie moléculaire Expériences. Biologie Expériences. ultrastructure. aat molecular structure. aat SCIENCE Life Sciences Cell Biology. bisacsh Biology Experiments fast Cytology Experiments fast Fourier transformations fast Imaging systems in biology fast Molecular biology Experiments fast Molecular structure fast Ultrastructure (Biology) fast |
| topic_facet | Ultrastructure (Biology) Molecular structure. Fourier transformations. Imaging systems in biology. Cytology Experiments. Molecular biology Experiments. Biology Experiments. Molecular Structure Ultrastructure (Biologie) Structure moléculaire. Imagerie en biologie. Cytologie Expériences. Biologie moléculaire Expériences. Biologie Expériences. ultrastructure. molecular structure. SCIENCE Life Sciences Cell Biology. Biology Experiments Cytology Experiments Fourier transformations Imaging systems in biology Molecular biology Experiments Molecular structure |
| url | https://search.ebscohost.com/login.aspx?direct=true&scope=site&db=nlebk&AN=454382 |
| work_keys_str_mv | AT moorepeter visualizingtheinvisibleimagingtechniquesforthestructuralbiologist |