Samer Gozem

Dr. Samer Gozem


Research Focus & Metrics

Academic Career Length

19Years (2008-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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30 October 2017 in Chemical Reviews
Verified
Journal Article
Closed access
SGSamer Gozem
Samer Gozem
HLHoi Ling Luk
Hoi Ling Luk
ISIgor Schapiro
Igor Schapiro
MOMassimo Olivucci
Massimo Olivucci

11 June 2014 in Journal of Chemical Theory and Computation
Verified
Journal Article
Closed access
SGSamer Gozem
Samer Gozem
FMFederico Melaccio
Federico Melaccio
AVAlessio Valentini
Alessio Valentini
MFMichael Filatov
Michael Filatov
MHMiquel Huix-Rotllant
Miquel Huix-Rotllant
MOMassimo Olivucci
Massimo Olivucci

24 September 2012 in Journal of Chemical Theory and Computation
Verified
Journal Article
Closed access
SGSamer Gozem
Samer Gozem
MHMark Huntress
Mark Huntress
ISIgor Schapiro
Igor Schapiro
RLRoland Lindh
Roland Lindh
AGAlexander A. Granovsky
Alexander A. Granovsky
MOMassimo Olivucci
Massimo Olivucci

13 November 2015 in Journal of Chemical Theory and Computation
Verified
Journal Article
Open access
DTDeniz Tuna
Deniz Tuna
DLDaniel Lefrancois
Daniel Lefrancois
Łukasz WolańskiŁukasz Wolański
Łukasz Wolański
SGSamer Gozem
Samer Gozem
ISIgor Schapiro
Igor Schapiro
MOMassimo Olivucci
Massimo Olivucci
As a minimal model of the chromophore of rhodopsin proteins, the penta-2,4-dieniminium cation (PSB3) poses a challenging test system for the assessment of electronic-structure methods for the exploration of ground- and excited-state potential-energy surfaces, the topography of conical intersections, and the dimensionality (topology) of the branching space. Herein, we report on the performance of the approximate linear-response coupled-cluster method of second order (CC2) and the algebraic-diagrammatic-construction scheme of the polarization propagator of second and third orders (ADC(2) and ADC(3)). For the ADC(2) method, we considered both the strict and extended variants (ADC(2)-s and ADC(2)-x). For both CC2 and ADC methods, we also tested the spin-component-scaled (SCS) and spin-opposite-scaled (SOS) variants. We have explored several ground- and excited-state reaction paths, a circular path centered around the S1/S0 surface crossing, and a 2D scan of the potential-energy surfaces along the branching space. We find that the CC2 and ADC methods yield a different dimensionality of the intersection space. While the ADC methods yield a linear intersection topology, we find a conical intersection topology for the CC2 method. We present computational evidence showing that the linear-response CC2 method yields a surface crossing between the reference state and the first response state featuring characteristics that are expected for a true conical intersection. Finally, we test the performance of these methods for the approximate geometry optimization of the S1/S0 minimum-energy conical intersection and compare the geometries with available data from multireference methods. The present study provides new insight into the performance of linear-response CC2 and polarization-propagator ADC methods for molecular electronic spectroscopy and applications in computational photochemistry.

31 May 2021 in WIREs Computational Molecular Science
Verified
Journal Article
Closed access
PDF file
SGSamer Gozem
Samer Gozem
AKAnna I. Krylov
Anna I. Krylov

4 November 2015 in The Journal of Physical Chemistry Letters
Verified
Journal Article
Open access
SGSamer Gozem
Samer Gozem
AGAnastasia O. Gunina
Anastasia O. Gunina
TITakatoshi Ichino
Takatoshi Ichino
DODavid L. Osborn
David L. Osborn
JSJohn F. Stanton
John F. Stanton
AKAnna I. Krylov
Anna I. Krylov
The calculation of absolute total cross sections requires accurate wave functions of the photoelectron and of the initial and final states of the system. The essential information contained in the latter two can be condensed into a Dyson orbital. We employ correlated Dyson orbitals and test approximate treatments of the photoelectron wave function, that is, plane and Coulomb waves, by comparing computed and experimental photoionization and photodetachment spectra. We find that in anions, a plane wave treatment of the photoelectron provides a good description of photodetachment spectra. For photoionization of neutral atoms or molecules with one heavy atom, the photoelectron wave function must be treated as a Coulomb wave to account for the interaction of the photoelectron with the +1 charge of the ionized core. For larger molecules, the best agreement with experiment is often achieved by using a Coulomb wave with a partial (effective) charge smaller than unity. This likely derives from the fact that the ef...