3.20 References 201 very important, since having a strong dipole perpendicular to the chain axis shows remarkable pyro and piezoelectric properties widely used in modern technology. According to Dwey-Aharon when the conformationally disordered material existing in form I1 is placed in a strong electric field (poling) conformational twistons are generated which propagate and yield form I. The spectroscopy of polyvynilidene fluoride and the search for twistons has been treated in [171]. Finally, the concept of twiston has been again introduced in a spectroscopic work to account for the set of peculiar experimental data collected in the study of the phase transition in ethylene-tetrafluoroethylene alternating copolymers [ 1721. Acknowledgments The contributions to knowledge presented in this chapter are the result of an enthusiastic collaboration of many researchers and students who worked in our group at the Politecnico of Milano. Our warmest thanks are extended to Dr. M. Gussoni, who laid the background for the development of this science. 3.20 References [l] H. H. Nielsen, Ha?idbzrclz der Plzvsik, Springer, Berlin, Vol. 37/1, 1959. [2] G. Herzberg, Infrared and Ranian <strong>Spect</strong>ra of’ Polyatonzic Molecules, Van Nostrand, Princeton, USA, 1963. [3] E. B. Wilson, J. C. Decius and P. C. Cross, Moleculur I/ibrutioiis, McGraw Hill, New York, 1955; V. Volkenstein, M. A. Eliashevich and B. Stepanov, Kolebuni.vu Molecul 11, Moscow, 1949; S. Califano, Vibrational Stutes, Wiley, New York, USA, 1976. [4] For a general discussion see: W. Person and G. Zerbi (Eds.), Vibrotional61teizsities in Infrared and Ranm <strong>Spect</strong>roscopy, Elsevier, Amsterdam, The Netherlands, 1984; L. A. Gribov, Intensity Theory for IIfrared <strong>Spect</strong>ra of Polyatoniic Molecarles, Consulting Bureau, New York, USA, 1964. [5] M. Gussoni in Aduances in hfiared and Ru~nan <strong>Spect</strong>roscopy, (Eds. R. J. H. Clark and R. H. Hester) Heyden, London, England, 1979, vol. 6 p. 96. [6] M. Gussoni, C. Castiglioni and G. Zerbi, J. Mol. Strzrct, 1989 198, 475 M. Gussoni, C. Castiglioni, M. N. Ramos, M. Rui and G. Zerbi, J. Mol. Strirct. 1990 224, 225 C. Decius, J. Mol. <strong>Spect</strong>ry, 57, 384 1975; A. J. Van Straten and W. Smit, .I Mol. <strong>Spect</strong>ry., 1976 62, 297 M. Gussoni, C. Castiglioni and G. Zerbi, J. Phys. Clienz. 1984 88, 600. [7] S. Trevino and H. Boutin, J. Macronzol. Sci., 1967 Al, 723. [8] E. Curtis, Thesis, University of Minnesota, 1958. [9] J. H. Schachtschneider and R. G. Snyder, <strong>Spect</strong>rocki/n. Acro, 1963 19, 17. [lo] The most known set of original computing programs which has later originated many other programs for dynamical and force constant calculations is that written by J. H. Schachtschneider, Shell Rep. 57/65. [ 111 See, for instance, J. L. Duncan, Force Curisfunt Calcirlcrtions ik hfokecirles, Specialist Report, Chemical Society, London, 1975, vol. 23, p. 104: G, Fogardsi and P. Pulay, in I’ihr.trtiorm/ <strong>Spect</strong>ru cind Strircfure, (Ed. J. R. Durig) Elsevier, Amsterdam, 1985, Vol. 14, p. 125.
202 3 Vibrutioncil <strong>Spect</strong>ra CIS a Probe of Striicturnl Odcr [I21 M. Gussoni, C. Castiglioni and G. Zerbi, J. Phys. Clzenr., 1984 88, 600. [I31 M. Gussoni, M. Ramos, C. Castiglioni and G. Zerbi, J. Mol. Struct., 1988 174, 47. [ 141 P. Pulay, X. Zhou and G. Fogarasi, in Rewit E~~~~ei~inientrd and Co/iif~/ittrtion[/I Atluirrrc,cc. i~7 Molecular <strong>Spect</strong>roscopy, (Ed. R: Fausto), NATO AS1 Series C, Vol. 406, p. 99; W. B. Person. K. Szczesniak and J. E. Del Bene, ibidem, p. 141. [I51 K. Palmo, L.-0. Pietila and S. Krimm, Conzpurers Clienz., 1991 f>, 249; K. Palmd, L.-0. Pietila and S. Krirniii. .I. Comp. Cl~eni., 1991 12, 385; K. Palmo, N. G. Mirkin, L.-0. Pieti13 and S. Krimni, M~momulecziles, 1993 26, 6831, K. Palmo, L.-0. Pietila and S. Krimm, computer.^ Clieni., 1993 17, 67; K. Palmo, L.-0. Pietila and S. Krimni, J. Comp. Clwnr.. 1992 13, 1142. [16] G. Zerbi, Vihrcitional <strong>Spect</strong>ra qf High Pol~wers, (Ed. E. G. Brame), Applied <strong>Spect</strong>roscopy Reviews. Dekker, New York, USA, 1963, vol. 2, p. 193; H. Tadokoro; Srrirc.trrw uf'Crj~stir1- lii7e Pol~~ers, Wiley, New York. 1979. [I71 P. C. Painter, M. M. Coleman and J. L. Koenig. Tlie Tlreury of t'ihutiond S)c,c.fro.cc'opj7' ctr7d its Applications to <strong>Polymer</strong>ic Materials, Wiley, New York, USA, 1982. [I81 For a general discussion of the dynamics of simple and simplified chain molecules see: R. Zbinden, Znjiaved <strong>Spect</strong>roscopy of High Poljvners, Academic, New York, USA. 1964. [ 191 G. Zerbi, Vibrational Sliectroscopy of Very Largt, molerirles, in Advances in Infrared and Rainan <strong>Spect</strong>roscopy (Eds. R. J. H. Clark and R. H. Hesterj Wiley-Heyden, New York, USA, vol. 11, p. 301. [20] J. C. Decius and R. M. Hexter, Moleciilar I4bratians in Crystcils, McGraw-Hill, New Yorb, 1977; S. Califano, V. Schettino and N. Neto, Lattice Dynnmics of i2.loleciilrrr Cr~.sfa/s. Lectut-e Notes in Chemistry, Springer, Berlin, 1981. 1211 M. Gussoni, G. Dellepiane and S. Abbate, J. Mol. <strong>Spect</strong>ry., 1975 57, 321. [22] For a discussion on the problem of redundancies see: M. Gussoni and G. Zerbi, Accademia Nazionale dei Lincei, Rendiconti serie VZZI 1966 40, 843; M . Gussoni and G. Zerbi, ibid. p. 1032; M. Gussoni and G. Zerbi, Clieni. PIiys. Lett., 1968 2, 145: I. M. Milk Clwni. Pliys. Lett. 1969 3, 267; G. Zerbi, in <strong>Modern</strong> Trends in I'ibrationul <strong>Spect</strong>roscop?', (Eds. A. J. Barnes and W. J. Orville-Thomas) Elsevier, Amsterdam. 1977. p. 261: M. V. Volkenstein, L. A. Gribov, M. A. Eliashevich and B. Stepanov, Kolehzniyci Molt~kul, Moskow, 1972, p. 203. [23] N. B. Colthup, L. H. Daly and S. E. Wiberley, Introdwtioii to Znfifi.arei/ and Xtnncirr S,ut*c./roscopy Academic, New York, 1975. [24] R. N. Jones and C. Sandorfy, Clienrical Applicntions uf Spec~troscopj~, in Teclmiques of Organic Chemistry, (Ed. A. Weissenberger) Interscience, New York, USA, 1956, vol. IX. [25] L. Bellaniy, The hfr~irt~l Slwctriz of COn711kY Moleciiles, Wiley, New Yo]-k, USA, 195s. 1261 K. Nakamoto, /nj?ared <strong>Spect</strong>ru of Polyatornic Molecules, Wiley, New York, 1963. [27] See the series of papers such as, for example, T. Shinianouchi, Tables qf Moleczrltrr Frcquencies, Part 7, J. Physicul and Cheniical Reference Dota, 1973 2, 225. [28] For the case of a polymer see, for instance, G. Masetti, S. Abbate, M. Gussoni and G. Zerbi. J. Clzern. Pliys. 1980 73, 4671. [29] M. Gussoni and G. Zerbi. J. &lo/. <strong>Spect</strong>ry., 1968 26, 485. [30] G. Dellepiane, M. Gussoni and G. Zerbi, J, Chern. Plqis. 1970 53, 3450; M. Gussoni, G. Dellepiane and G. Zerbi, in Molecular Structures and I'lbrations (Ed. S. J. Cyvin) Elsevier, Amsterdam, 1972, p. 101. [31] P. Torkington, J. Cliern. Phylys., 1949 17, 347. [32] Y. Morino and K. Kuchitsu, J. cheni. Plz-vs., 1952 20, 1809. [33] J. H. Schachtschneider and R. G. Snyder, <strong>Spect</strong>rochini. Actu 1963, 19, 17. [34] R. G. Snyder and J. H. Schachtschneider, Sj7ectrocliim. Acta. 1963 19, 117. [35] J. H. Schachtschneider and R. G. Snyder, <strong>Spect</strong>rocliim. ACIU, 1965 21, 1527. [36] R. G. Snyder, J. Clwrn. Phys., 1967 47, 1316. 1371 R. G. Snyder and G. Zerbi, <strong>Spect</strong>roclrini. Acta, 1967 23 A, 391. [38] W. T. King and B. L. Crawford, J. Mol. <strong>Spect</strong>ry., 1960 5, 429. [39] J. Overend and J. R. Scherer, Spc.c.trocAini. Actrt, 1960 16, 773. [40] Handbook of Conducting Polyniers, (Ed. T. A. Skotheini) Dekker? New York. 1986. Vols. I and 2.
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Modern Polymer Spectroscopy Edited
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Modern Polymer Spectroscopy Edited
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Preface For unfortunate reasons the
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However, theory and calculations yi
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Contents 1 Two-Dimensional Infrared
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Con ten t~ xi Index 5.2 Force Field
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Contributors M. Del Zoppo Dipartime
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1 Two-Dimensional Infrared (2D IR)
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1.2 Brick~qrorrnrl 3 . Figure 1-3.
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1.0 , Figure 1-6. The in-phtrse and
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1.2 Bcrckgroinizd 7 where AA (i~) i
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1.2 Background 9 1.2.5 Two-Dimensio
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1.3 Bnsic Properties of 20 IR Corre
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2D IR spectrometer coupled with a d
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1.5 Applirtrtions 15 Unlike a dispe
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\ '\ Melliyleiie 1'7- -3000 Posiliv
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11 Amorphous Crystalline ,...." I F
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1.5 Applications 21 / I 1430 Figure
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1.5 Appliccitioiis 23 Methylene Fig
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1.5 Ajqdicrrtions 25 3024 Figure 1-
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1.5 Applicutions 27 Furthermore. th
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1.7 Coizclirsions 29 derived in a s
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1.9 References 31 [9] Colthup, N. B
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2 Segmental Mobility of Liquid Crys
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SRMPLE/DETECTOR e3 ‘retardation
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2.4 Srvuc me-Dependenr Alignment 37
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2.5 Electric Field-Innductid Orirnt
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2.5 Electric Field-nclticetl Orient
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a -@ COWER SRHPLE ._ 2.5 Elec tric
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2.5 Electric Field-Itzduced Orienta
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2.5 Electric Field-IwrElrced Orient
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2.5 Electric Field-Im/irced Orientu
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2.5 Electric Field-Induced Orientli
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2.5 Electric Field-Induced Orientat
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2.5 Electric Field-Induced Orienfat
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2.5 Elrc tric Field-Iiidircwl Orim
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2500 2008 I s00 WRVtNdMRtR CM-I Fig
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-3.6 Aligmient OJ' Side- Clinin Liy
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~ polyester 2.6 Alignnient qf Side-
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I." 0.9 0.8 Figure 2-34. FTlR 0.7 p
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induced alignment of the investigat
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2.7 Orientation oj Liquid Ci:i,stal
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2.7 Orieritation of Liquid Ciysttrl
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0 8 18 16 1 a W u z a m a 0 Ln m Q
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2.7 Orientation oj Liquid Crystals
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2.7 Orientation of Liquid Crjvtals
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2.7 Orientatioiz of Liquid Crystals
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2.8 Conclusions 81 strain. As A0 is
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3. I0 Refcreiice.r 83 [I 71 Hoffina
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2.10 References 85 [92] Wiesner, U.
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t Order/Disorder in Chain Molecules
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onds which hold atoms together thro
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3.2 The Dyriamical Case qf Simll ar
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3.2 The Dyrinniical Case of Sinnll
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3.4 S11or.f- and Loizg-Rcrizye Vibr
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3.4 Slzort- and Loiig-Range Vibrati
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eyularity), e.g., 2. During the pol
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3.5 Towards Lnrger Molecules: From
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3.5 TOIIYW~ Laiyer Molertiles: Fvoi
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3.5 Towmu" Larger Molecules: F~om O
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1700 - CIO --- ca c 22 _- c 12 l l
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3.6 From Dynamics to Vibrational Sp
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3.6 Froin Dynaiiiics to T’ihratio
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3.7 The Case of Isotactic Polypropy
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3.7 The Cuse of Isotactic Polypvop.
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3.8 Density of Vibrational States a
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3.8 Dtvz.sit,v of L’ihrntioizal S
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3.8 Driisity of Vibratioiid StLitrs
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3 9 Mouiiiq ToIvmds Rerrlitv: From
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3.9 Moving Towards Reality: From Or
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3.9 Moving Towards Reality: Froin O
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3.10 Wlmt Do We Learn from Cnlcailc
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+ 3.11 A Very Siriiple Ccrse: Latti
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3 I1 A Yey) Siiiiple Case: LLittice
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3.11 A Vq> Siiiiplc Crrw: Luttice D
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Figure 3-22. Sample eigenvectors in
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3.12 CIS-trans Opening @the Double
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3.13 Defect Modes cis Structtrr.al
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3.13 Defect Mo&s cis Structurcil Pr
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0 3.14 Case Studies N 0 d - Y N o m
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3.14 Case Studies 147 OC 60 58 57.
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3.14 Case Studies 149 GI A V E N U
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5.3 Ainide Modes 251 Table 5-1. Ami
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Table 5-2. Some amide modes of four
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5.3 Amidc Modes 255 Figure 5-1. Opt
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5.4 Polypeptides 257 nonhydrogen-bo
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5.4 Polvpeptida 259 Figure 5-2. Ant
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I 5.4 Polypeptides 261 )I .- + $ 80
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1226M 1222s (1 1165W 1167s (1 1120V
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135s 9 1 Ms1i 122Wbr 147 NH ob(37)
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5.4 Polypeptides 267 glycine residu
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5.4 Polypeptides 269 Raman bands in
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5.4 Polypeptides 271 Figure 5-7. St
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Frequency (cm-'1 100% b 700 500 300
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5.4 Polypptidt~s 215 Table 5-9. Obs
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~~ ~~ ~~~ ~ ~ ~~ 5.4 Polypeptides 2
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5.4 Poliyeptides 219 Table 5-11. Co
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Table 5-12. Aniide mode frequencies
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1351 Lifson, S., Stern, P. S., J. C
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5.6 Refeverices 285 [130] Tiffany,
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Index Amide modes 249 Amorphous pol
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Step-scan FTIR spectroscopy 14,34 -