Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs

Effective polarizabilities of Na(NH<inf>3</inf>)<inf>n</inf> (n = 8-27) clusters were measured by electric deflection as a function of the particle size. A significant field-induced shift of the beam intensity profile without the occurrence of broadening revealed that the clu...

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Autores principales: Carrera, A., Marceca, E.
Formato: JOUR
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_10895639_v119_n18_p4207_Carrera
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spelling todo:paper_10895639_v119_n18_p4207_Carrera2023-10-03T16:04:49Z Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs Carrera, A. Marceca, E. Ammonia Particle size Ammonia clusters Beam intensity profile Cluster temperature Electric deflection Polarizabilities Solvation process Unpaired electrons Valence electron Solvents Effective polarizabilities of Na(NH<inf>3</inf>)<inf>n</inf> (n = 8-27) clusters were measured by electric deflection as a function of the particle size. A significant field-induced shift of the beam intensity profile without the occurrence of broadening revealed that the clusters behave as liquidlike polar objects in the conditions of the experiment (cluster temperatures were estimated in the range of 110-145 K). Most of the cluster polarity is attributed to the spontaneous promotion of the alkali atom valence electron to a diffuse state stabilized by the cluster solvent field, with the consequent formation of (e-, Na+) pairs. The average modulus of the dipole of Na-NH<inf>3</inf> clusters, μ<inf>0</inf>, was determined using the Langevin-Debye theory, and the data was compared with previous measurements obtained for Na-H<inf>2</inf>O clusters. Sodium-doped ammonia clusters exhibit much larger μ<inf>0</inf> values and a step size dependence which is not present when the solvent is water. This evidence suggests that while the (e-, Na+) structure is rather compact in Na(H<inf>2</inf>O)<inf>n</inf> clusters and remains almost unchanged during the solvation process, in Na(NH<inf>3</inf>)<inf>n</inf> the unpaired electron abandons the proximity of the Na+ ion and gradually extends and occupies new solvent shells. © 2015 American Chemical Society. Fil:Carrera, A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. Fil:Marceca, E. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_10895639_v119_n18_p4207_Carrera
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Ammonia
Particle size
Ammonia clusters
Beam intensity profile
Cluster temperature
Electric deflection
Polarizabilities
Solvation process
Unpaired electrons
Valence electron
Solvents
spellingShingle Ammonia
Particle size
Ammonia clusters
Beam intensity profile
Cluster temperature
Electric deflection
Polarizabilities
Solvation process
Unpaired electrons
Valence electron
Solvents
Carrera, A.
Marceca, E.
Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs
topic_facet Ammonia
Particle size
Ammonia clusters
Beam intensity profile
Cluster temperature
Electric deflection
Polarizabilities
Solvation process
Unpaired electrons
Valence electron
Solvents
description Effective polarizabilities of Na(NH<inf>3</inf>)<inf>n</inf> (n = 8-27) clusters were measured by electric deflection as a function of the particle size. A significant field-induced shift of the beam intensity profile without the occurrence of broadening revealed that the clusters behave as liquidlike polar objects in the conditions of the experiment (cluster temperatures were estimated in the range of 110-145 K). Most of the cluster polarity is attributed to the spontaneous promotion of the alkali atom valence electron to a diffuse state stabilized by the cluster solvent field, with the consequent formation of (e-, Na+) pairs. The average modulus of the dipole of Na-NH<inf>3</inf> clusters, μ<inf>0</inf>, was determined using the Langevin-Debye theory, and the data was compared with previous measurements obtained for Na-H<inf>2</inf>O clusters. Sodium-doped ammonia clusters exhibit much larger μ<inf>0</inf> values and a step size dependence which is not present when the solvent is water. This evidence suggests that while the (e-, Na+) structure is rather compact in Na(H<inf>2</inf>O)<inf>n</inf> clusters and remains almost unchanged during the solvation process, in Na(NH<inf>3</inf>)<inf>n</inf> the unpaired electron abandons the proximity of the Na+ ion and gradually extends and occupies new solvent shells. © 2015 American Chemical Society.
format JOUR
author Carrera, A.
Marceca, E.
author_facet Carrera, A.
Marceca, E.
author_sort Carrera, A.
title Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs
title_short Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs
title_full Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs
title_fullStr Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs
title_full_unstemmed Electric deflection of middle-size ammonia clusters containing (e-, Na+) Pairs
title_sort electric deflection of middle-size ammonia clusters containing (e-, na+) pairs
url http://hdl.handle.net/20.500.12110/paper_10895639_v119_n18_p4207_Carrera
work_keys_str_mv AT carreraa electricdeflectionofmiddlesizeammoniaclusterscontainingenapairs
AT marcecae electricdeflectionofmiddlesizeammoniaclusterscontainingenapairs
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