Louis Schlapbach
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Louis Schlapbach has a total of 538 co-authors. Here are the top co-authors by number of shared publications:
J. Osterwalder
Physik-Institut Universität Zürich-Irchel, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
53 shared publicationsP. Aebi
Institut de Physique, Université de Neuchâtel, CH-2000 Neuchâtel, Switzerland
51 shared publicationsP. Gröning
Physics Department, University of Fribourg, Pérolles, CH-1700 Fribourg, Switzerland
34 shared publicationsAndreas Züttel
EMPA, Swiss Federal Laboratories for Materials Research and Testing, CH-8600 Dübendorf, Switzerland
23 shared publications- Thomas Greber
Physik-Institut, University of Zurich, Zurich, Switzerland
22 shared publications D. Naumović
Département de Physique, Université de Fribourg, Pérolles, CH-1700 Fribourg, Switzerland
19 shared publications
Latest Publications
- Open Access
- 1 September 2015
- Published by Elsevier in Journal of Materiomics
- Vol. 1 (3) , 196-204
Enhanced thermoelectric properties of samarium boride
- 1 September 2015
- Published by Elsevier in Journal of Materiomics
- Vol. 1 (3) , 196-204
Open AccessEnhanced thermoelectric properties of samarium boride
- 1 October 2010
- Published by World Scientific Pub Co Pte Ltd
- p. 265-270
Hydrogen-storage materials for mobile applications
- 1 October 2010
- Published by World Scientific Pub Co Pte Ltd
- p. 265-270
Hydrogen-storage materials for mobile applications
- 12 August 2009
- Published by Springer Nature in Nature
- Vol. 460 (7257) , 809-811
Hydrogen-fuelled vehicles
- 12 August 2009
- Published by Springer Nature in Nature
- Vol. 460 (7257) , 809-811
Hydrogen-fuelled vehicles
- 1 July 2008
- Published by Elsevier in Physica B: Condensed Matter
- Vol. 403 (13-16) , 2207-2210
Atomic origin of the scanning tunneling microscopy images of charge-density-waves on 1T-TaSe2
- 1 July 2008
- Published by Elsevier in Physica B: Condensed Matter
- Vol. 403 (13-16) , 2207-2210
Atomic origin of the scanning tunneling microscopy images of charge-density-waves on 1T-TaSe2
- 17 September 2007
- Published by American Physical Society (APS) in Physical Review B
- Vol. 76 (12) , 125205
Formation of electron traps in amorphous silica
The capture of an electron by a silicon atom in a defect-free bulk of amorphous silica has been investigated. Ab initio constrained dynamics has been applied to evaluate the energy barrier. The computed energy barrier involved in the mechanism was found to be . The electron trapping is accompanied by a strong local distortion of the tetrahedron of and involved in the process. Hydrogen, which is an electronically active impurity of silicon dioxide, bonds to the oxygen of the silica bond on which the electron is localized. Upon restoring the neutrality of the system a paramagnetic configuration is found. The eigenvalues of the hyperfine tensor have been evaluated.- 17 September 2007
- Published by American Physical Society (APS) in Physical Review B
- Vol. 76 (12) , 125205
Formation of electron traps in amorphous silica
The capture of an electron by a silicon atom in a defect-free bulk of amorphous silica has been investigated. Ab initio constrained dynamics has been applied to evaluate the energy barrier. The computed energy barrier involved in the mechanism was found to be . The electron trapping is accompanied by a strong local distortion of the tetrahedron of and involved in the process. Hydrogen, which is an electronically active impurity of silicon dioxide, bonds to the oxygen of the silica bond on which the electron is localized. Upon restoring the neutrality of the system a paramagnetic configuration is found. The eigenvalues of the hyperfine tensor have been evaluated.- Open Access
- 21 August 2007
- Published by American Physical Society (APS) in Physical Review B
- Vol. 76 (7) , 073410
Tunneling evidence for spatial location of the charge-density-wave induced band splitting inWe present the atomically resolved room temperature scanning-tunneling microscopy study of bias dependent images of charge density waves (CDWs) in . With the help of angle-resolved photoemission of the CDW-split band in , we determine the electronic location of subbands on inequivalent atoms of the reconstructed Ta plane. We thus demonstrate the atomic origin of the CDW-formation related effects observed in the band structure of this material.- 21 August 2007
- Published by American Physical Society (APS) in Physical Review B
- Vol. 76 (7) , 073410
Open AccessTunneling evidence for spatial location of the charge-density-wave induced band splitting inWe present the atomically resolved room temperature scanning-tunneling microscopy study of bias dependent images of charge density waves (CDWs) in . With the help of angle-resolved photoemission of the CDW-split band in , we determine the electronic location of subbands on inequivalent atoms of the reconstructed Ta plane. We thus demonstrate the atomic origin of the CDW-formation related effects observed in the band structure of this material. - 1 October 2003
- Published by Springer Nature in Analytical and Bioanalytical Chemistry
- Vol. 377 (3) , 578-586
Cell spreading on quartz crystal microbalance elicits positive frequency shifts indicative of viscosity changes
Cell attachment and spreading on solid surfaces was investigated with a home-made quartz crystal microbalance (QCM), which measures the frequency, the transient decay time constant and the maximal oscillation amplitude. Initial interactions of the adsorbing cells with the QCM mainly induced a decrease of the frequency, coincident with mass adsorption. After about 80 min, the frequency increased continuously and after several hours exceeded the initial frequency measured before cell adsorption. Phase contrast and fluorescence microscopy indicated that the cells were firmly attached to the quartz surface during the frequency increase. The measurements of the maximal oscillation amplitude and the transient decay time constant revealed changes of viscoelastic properties at the QCM surface. An important fraction of these changes was likely due to alterations of cytosolic viscosity, as suggested by treatments of the attached cells with agents affecting the actin and microtubule cytoskeleton. Our results show that viscosity variations of cells can affect the resonance frequency of QCM in the absence of apparent cell desorption. The simultaneous measurements of the maximal oscillation amplitude, the transient decay time constant and the resonance frequency allow an analysis of cell adsorption to solid substratum in real time and complement cell biological methods.
- 1 October 2003
- Published by Springer Nature in Analytical and Bioanalytical Chemistry
- Vol. 377 (3) , 578-586
Cell spreading on quartz crystal microbalance elicits positive frequency shifts indicative of viscosity changes
Cell attachment and spreading on solid surfaces was investigated with a home-made quartz crystal microbalance (QCM), which measures the frequency, the transient decay time constant and the maximal oscillation amplitude. Initial interactions of the adsorbing cells with the QCM mainly induced a decrease of the frequency, coincident with mass adsorption. After about 80 min, the frequency increased continuously and after several hours exceeded the initial frequency measured before cell adsorption. Phase contrast and fluorescence microscopy indicated that the cells were firmly attached to the quartz surface during the frequency increase. The measurements of the maximal oscillation amplitude and the transient decay time constant revealed changes of viscoelastic properties at the QCM surface. An important fraction of these changes was likely due to alterations of cytosolic viscosity, as suggested by treatments of the attached cells with agents affecting the actin and microtubule cytoskeleton. Our results show that viscosity variations of cells can affect the resonance frequency of QCM in the absence of apparent cell desorption. The simultaneous measurements of the maximal oscillation amplitude, the transient decay time constant and the resonance frequency allow an analysis of cell adsorption to solid substratum in real time and complement cell biological methods.
- 1 October 2003
- Published by Springer Nature in Analytical and Bioanalytical Chemistry
- Vol. 377 (3) , 570-577
Simultaneous measurement of the maximum oscillation amplitude and the transient decay time constant of the QCM reveals stiffness changes of the adlayer
Interpretation of adsorption kinetics measured with a quartz crystal microbalance (QCM) can be difficult for adlayers undergoing modification of their mechanical properties. We have studied the behavior of the oscillation amplitude, A 0, and the decay time constant, τ, of quartz during adsorption of proteins and cells, by use of a home-made QCM. We are able to measure simultaneously the frequency, f, the dissipation factor, D, the maximum amplitude, A 0, and the transient decay time constant, τ, every 300 ms in liquid, gaseous, or vacuum environments. This analysis enables adsorption and modification of liquid/mass properties to be distinguished. Moreover the surface coverage and the stiffness of the adlayer can be estimated. These improvements promise to increase the appeal of QCM methodology for any applications measuring intimate contact of a dynamic material with a solid surface.
- 1 October 2003
- Published by Springer Nature in Analytical and Bioanalytical Chemistry
- Vol. 377 (3) , 570-577
Simultaneous measurement of the maximum oscillation amplitude and the transient decay time constant of the QCM reveals stiffness changes of the adlayer
Interpretation of adsorption kinetics measured with a quartz crystal microbalance (QCM) can be difficult for adlayers undergoing modification of their mechanical properties. We have studied the behavior of the oscillation amplitude, A 0, and the decay time constant, τ, of quartz during adsorption of proteins and cells, by use of a home-made QCM. We are able to measure simultaneously the frequency, f, the dissipation factor, D, the maximum amplitude, A 0, and the transient decay time constant, τ, every 300 ms in liquid, gaseous, or vacuum environments. This analysis enables adsorption and modification of liquid/mass properties to be distinguished. Moreover the surface coverage and the stiffness of the adlayer can be estimated. These improvements promise to increase the appeal of QCM methodology for any applications measuring intimate contact of a dynamic material with a solid surface.
- 21 August 2003
- Published by Wiley in Advanced Engineering Materials
- Vol. 5 (8) , 541-550
Carbon Nanotubes for Cold Electron Sources
Technological advances in the field of microelectronic fabrication techniques have triggered a great interest in vacuum microelectronics. In contrast to solid‐state microelectronics, which entails scattering‐dominated electron transport in semiconducting solids, vacuum microelectronics relies on the scattering‐free, ballistic motion of electrons in vacuum. Since the first international conference on vacuum microelectronics substantial progress in this field has been made. The first technological devices using micrometer‐sized electron emitting structures are currently being commercialized. Field‐emission flat‐panel displays (FED) seem to be an especially promising competitor to LCD displays. Today there is only one mature technology for producing micro‐gated field‐emission arrays: the Spindt metal‐tip process. The drawbacks of this technology are expensive production, critical lifetime in vacuum, and high operating voltage. Carbon nanotubes (CNT) can be regarded as the potential second‐generation technology to the Spindt metal micro‐tip. In this review we show that the field emission (FE) behavior of CNT can be accurately described by Fowler–Nordheim tunneling and that the field‐enhancement factor β is the most prominent factor. Therefore the FE properties of a CNT thin film can be understood in terms of local field enhancement β(x,y), which can be determined with scanning anode field emission microscopy (SAFEM). To characterize the FE properties of an ensemble of electron emitters we used a statistical approach (as for thin film emitters), where f(β)dβ gives the number of emitters on a unit area with field‐enhancement factors within the interval [β,β + dβ]. We show that the field‐enhancement distribution function f(β) gives an almost complete characterization of the FE properties.
- 21 August 2003
- Published by Wiley in Advanced Engineering Materials
- Vol. 5 (8) , 541-550
Carbon Nanotubes for Cold Electron Sources
Technological advances in the field of microelectronic fabrication techniques have triggered a great interest in vacuum microelectronics. In contrast to solid‐state microelectronics, which entails scattering‐dominated electron transport in semiconducting solids, vacuum microelectronics relies on the scattering‐free, ballistic motion of electrons in vacuum. Since the first international conference on vacuum microelectronics substantial progress in this field has been made. The first technological devices using micrometer‐sized electron emitting structures are currently being commercialized. Field‐emission flat‐panel displays (FED) seem to be an especially promising competitor to LCD displays. Today there is only one mature technology for producing micro‐gated field‐emission arrays: the Spindt metal‐tip process. The drawbacks of this technology are expensive production, critical lifetime in vacuum, and high operating voltage. Carbon nanotubes (CNT) can be regarded as the potential second‐generation technology to the Spindt metal micro‐tip. In this review we show that the field emission (FE) behavior of CNT can be accurately described by Fowler–Nordheim tunneling and that the field‐enhancement factor β is the most prominent factor. Therefore the FE properties of a CNT thin film can be understood in terms of local field enhancement β(x,y), which can be determined with scanning anode field emission microscopy (SAFEM). To characterize the FE properties of an ensemble of electron emitters we used a statistical approach (as for thin film emitters), where f(β)dβ gives the number of emitters on a unit area with field‐enhancement factors within the interval [β,β + dβ]. We show that the field‐enhancement distribution function f(β) gives an almost complete characterization of the FE properties.