LEADER 03286nam 2200577 a 450 001 9910437813103321 005 20200520144314.0 010 $a1-283-93564-3 010 $a3-7091-1317-2 024 7 $a10.1007/978-3-7091-1317-2 035 $a(CKB)2670000000317279 035 $a(EBL)1030790 035 $a(OCoLC)827616964 035 $a(SSID)ssj0000879268 035 $a(PQKBManifestationID)11461448 035 $a(PQKBTitleCode)TC0000879268 035 $a(PQKBWorkID)10852949 035 $a(PQKB)10881127 035 $a(DE-He213)978-3-7091-1317-2 035 $a(MiAaPQ)EBC1030790 035 $a(PPN)168331454 035 $a(EXLCZ)992670000000317279 100 $a20130108d2013 uy 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 00$aMaterial designs and new physical properties in MX- and MMX-chain compounds /$fMasahiro Yamashita, Hiroshi Okamoto, editors 205 $a1st ed. 2013. 210 $aWien ;$aNew York $cSpringer$dc2013 215 $a1 online resource (274 p.) 300 $aDescription based upon print version of record. 311 $a3-7091-1735-6 311 $a3-7091-1316-4 320 $aIncludes bibliographical references and index. 327 $apt. 1. MX-chain compounds -- pt. 2. MMX-chain compounds. 330 $aThis is the first book to comprehensively address the recent developments in both the experimental and theoretical aspects of quasi-one-dimensional halogen-bridged mono- (MX) and binuclear metal (MMX) chain complexes of Pt, Pd and Ni. These complexes have one-dimensional electronic structures, which cause the various physical properties as well as electronic structures. In most MX-chain complexes, the Pt and Pd units are in M(II)-M(IV) mixed valence or charge density wave (CDW) states due to electron-phonon interactions, and Ni compounds are in Ni(III) averaged valence or Mott-Hubbard states due to the on-site Coulomb repulsion. More recently, Pd(III) Mott-Hubbard (MH) states have been realized in the ground state by using the chemical pressure. Pt and Pd chain complexes undergo photo-induced phase transitions from CDW to MH or metal states, and Ni chain complexes undergo photo-induced phase transitions from MH to metal states. Ni chain complexes with strong electron correlations show tremendous third-order optical nonlinearity and nonlinear electrical conductivities. They can be explained theoretically by using the extended Peierls-Hubbard model. For MMX-chain complexes, averaged valence, CDW, charge polarization, and alternating charge polarization states have been realized by using chemical modification and external stimuli, such as temperature, photo-irradiation, pressure, and water vapor. All of the electronic structures and phase transitions can be explained theoretically. 606 $aMaterials$xDesign 615 0$aMaterials$xDesign. 676 $a541/.36 676 $a620.11299 701 $aYamashita$b Masahiro$01758197 701 $aOkamoto$b Hiroshi$0666163 801 0$bMiAaPQ 801 1$bMiAaPQ 801 2$bMiAaPQ 906 $aBOOK 912 $a9910437813103321 996 $aMaterial designs and new physical properties in MX- and MMX-chain compounds$94196356 997 $aUNINA