Carlos Manzano’s research while affiliated with Agency for Science, Technology and Research (A*STAR) and other places

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Publications (17)


Mapping the Excited States of Single Hexa-peri-benzocoronene Oligomers
  • Article

March 2012

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138 Reads

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28 Citations

ACS Nano

We-Hyo Soe

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Hon Seng Wong

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Carlos Manzano

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[...]

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Christian Joachim

Electronic states of a molecule are usually analyzed via their decomposition in linear superposition of multielectronic Slater determinants built up from monoelectronics molecular orbitals. It is generally believed that a scanning tunneling microscope (STM) is able to map those molecular orbitals. Using a low-temperature ultrahigh vacuum (LT-UHV) STM, the dI/dV conductance maps of large single hexabenzocoronene (HBC) monomer, dimer, trimer, and tetramer molecules were recorded. We demonstrate that the attribution of a tunnel electronic resonance to a peculiar π molecular orbital of the molecule (or σ intermonomer chemical bond) in the STM junction is inappropriate. With an STM weak-measurement-like procedure, a dI/dV resonance results from the conductance contribution of many molecular states whose superposition makes it difficult to reconstruct an apparent molecular orbital electron probability density map.


Origin of the apparent (2× 1) topography of the Si (100)-c (4× 2) surface observed in low-temperature STM images

May 2011

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44 Reads

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17 Citations

Physical review. B, Condensed matter

Low-temperature scanning tunneling microscope (STM) images of the Si(100) surface showing apparent (2×1) atom dimer lines have recently been reported. Using experimental and theoretical approaches, it is demonstrated how those (2×1)-like images result from a c(4×2) surface reconstruction imaged at high bias voltages. In the STM junction, the surface contribution of 3px surface-state electronic resonances relative to the 3pz states is bias voltage dependent. The apparent (2×1) STM images result from an increase in the number of bulk Si electronic channels amplifying Si(100)-c(4×2) surface 3px surface states contribution to the tunneling current with respect to the one of 3pz states.


FIG. 2. (Color online) (a) Simplified QHC molecule inserted between two electrodes. The two electrodes are supposed to interact only with the first state of the simplified molecule through the couplings V. These couplings are V = −0.15 eV. (b) The transmission coefficient of the system represented in (a) calculated with the ESQC technique for different values of the logical input (solid black line). The T (E) follows the same variation as the normalized oscillation frequency for the system represented in Fig. 1(a) (dashed blue line). The chemical potentials of the electrode define the integration region of the T (E) (grey shaded area) that gives the output current intensity.
FIG. 5. (Color online) Top: The three experimental images obtained approaching successively none, one, and two Au atoms near the end of the naphtyl branches. Middle: Molecular model of the Au-trinaphthylene surface system when optimizing its atomic scale surface structure for the experimental and calculated images to converge scan by scan. This optimization demonstrates the displacement of the H atoms when approaching a Au atom to the molecule. Bottom: The theoretical ESQC-STM images of the trinaphtylene interacting with none, one, and two surface atoms. 
FIG. 6. (Color online) Experimental and theoretical dI /dV map of the molecule recorded at the energy of the HOMO-1, HOMO, and LUMO of the system for zero, one, and two atoms interacting with the molecule. A good agreement is seen between experiment and theory. Experimental and theoretical images shows how approaching one atom in the vicinity of the molecule deforms nonlocally its molecular orbitals due to their delocalization over the molecular board. 
FIG. 7. (Color online) dI /dV spectra for the three nonequivalent Au-trinaphthylene molecule configurations. While a broad peak corresponding to the LUMO appears in all configurations at the positive bias, a distinct peak in the negative regime observed on a bare molecule is split and shifted by Au atom inputs. The HOMO of a molecule in gas phase, with a threefold symmetry, and the degenerated HOMO-1 and HOMO-2 orbitals, with twofold and mirror symmetries, are very close to the same energy level. However once adsorbed on a substrate this degeneracy unravels due to symmetry constrains resulting in the HOMO-2 orbital being dropped out from this energy range. Therefore the peak at − 1600 mV in the spectrum taken from a bare molecule consists of only HOMO and HOMO-1. The surface state of Au(111) is provided as a reference. 
FIG. 8. (Color online) I - V characteristics recorded by position- ing the tip apex at the output side of the molecule exactly at the maximum lobe position of the first resonance at negative bias voltage (HOMO). Four I - V characteristics were recorded corresponding to 0, 1, 1, and 2 Au input atoms at the in position. The absolute value of the current intensity is larger in the (0,0) case than in the three other case which is the requirement to obtain a NOR gate. 

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Demonstration of a NOR logic gate using a single molecule and two surface gold atoms to encode the logical input
  • Article
  • Full-text available

April 2011

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325 Reads

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40 Citations

Physical review. B, Condensed matter

A logic gate has been implemented in a single trinaphthylene molecule. Each logical input controls the position of a surface Au atom that is brought closer or further away from the end of one of the naphthyl branch. Each Au atom carries 1 bit of information and is able to deform nonlocally and to shift in energy the molecular electronic states of the trinaphthylene. Probed at the end of the third naphthyl branch using scanning tunneling spectroscopy, the variations of the tunneling current intensity as a function of the Au atoms position measures the logical output of the gate. We demonstrate both theoretically and experimentally that these variations respect the truth table of a NOR logic gate.

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Manipulating Molecular Quantum States with Classical Metal Atom Inputs: Demonstration of a Single Molecule NOR Logic Gate

February 2011

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52 Reads

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77 Citations

ACS Nano

Quantum states of a trinaphthylene molecule were manipulated by putting its naphthyl branches in contact with single Au atoms. One Au atom carries 1-bit of classical information input that is converted into quantum information throughout the molecule. The Au-trinaphthylene electronic interactions give rise to measurable energy shifts of the molecular electronic states demonstrating a NOR logic gate functionality. The NOR truth table of the single molecule logic gate was characterized by means of scanning tunnelling spectroscopy.


Step-by-step rotation of a molecule-gear mounted on an atomic-scale axis

August 2009

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119 Reads

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128 Citations

Nature Materials

Gears are microfabricated down to diameters of a few micrometres. Natural macromolecular motors, of tens of nanometres in diameter, also show gear effects. At a smaller scale, the random rotation of a single-molecule rotor encaged in a molecular stator has been observed, demonstrating that a single molecule can be rotated with the tip of a scanning tunnelling microscope (STM). A self-assembled rack-and-pinion molecular machine where the STM tip apex is the rotation axis of the pinion was also tested. Here, we present the mechanics of an intentionally constructed molecule-gear on a Au(111) surface, mounting and centring one hexa-t-butyl-pyrimidopentaphenylbenzene molecule on one atom axis. The combination of molecular design, molecular manipulation and surface atomic structure selection leads to the construction of a fundamental component of a planar single-molecule mechanical machine. The rotation of our molecule-gear is step-by-step and totally under control, demonstrating nine stable stations in both directions.


FIG. 1. A 10 : 0 nm  9 : 5 nm constant-current STM image of a pentacene molecule bound to a herringbone kink of the reconstructed Au(111) surface. The inset shows the apparent height profile taken along this pentacene molecule. Scanning conditions: I 1⁄4 45 pA , V 1⁄4 100 mV . 
Fig. 2(a). At a given position ( x , y ) and for a tip apex to surface distance z , I is given by e 2 Z E F þ eV I ð V; z Þ 1⁄4 T ð E; z Þ dE; (1) @ E F 
FIG. 2 (color online). (a) The dI=dV spectrum of a pentacene molecule on Au(111). The dI=dV signal shows four broad and distinct peaks corresponding to the first affinity level (LUMO) of a pentacene, in the positive bias side, and its one electron ionization levels (HOMO, HOMO-1, and lower) in the negative side. The leftmost peak certainly consists of two resonances, HOMO-2 and HOMO-3, but these are too close energetically to be resolved by spectroscopy in this high voltage region [13]. The surface state of Au(111) is also observable. (b) The left and center columns are experimental topographic images and dI=dV maps recorded at voltages indicated by the arrows in (a). Tunneling currents for the STM images and dI=dV maps are, from the top, 5 nA, 3 nA, 5 nA, and 6 nA. The right column displays the corresponding calculated STM-elastic scattering quantum chemistry (ESQC) images, at a constant tunneling current of 1 nA, for a pentacene molecule adsorbed on Au(111) at the monoelectronic energy resonances corresponding to the LUMO, HOMO, HOMO-1, and HOMO-2, respectively. All images are 2:5 nm  1:5 nm.
FIG. 3. (a) Topographic and (b) dI=dV images taken in the gap between the HOMO and HOMO-1 resonances ( V 1⁄4 À 1400 mV and I 1⁄4 4 nA ). (c) Constant-current ESQC-computed z map, at 1 nA. Here the integration performs from the Fermi energy to an energy lying exactly midway between the HOMO and HOMO-1. (d) ESQC-computed conductance map at E 1⁄4 ð E HOMO þ 
FIG. 4 (color online). A three-dimensional (3D) representation showing the contribution of resonant and nonresonant states explaining the dI=dV map recorded at À2500 mV. The three topmost 3D plots were extracted from the ESQC theoretical results shown in the right column of Fig. 2(b). The 3D plot at the bottom corresponds to the weighted sum of the HOMO-2, HOMO-1, and HOMO shown above. The criteria for the integration is (i) resonant states (HOMO-2 in this case) are positive, (ii) nonresonant states (HOMO and HOMO-1) are negative, and (iii) the nearer the Fermi energy, the stronger is the contribution of the nonresonant states [14]. The image at the bottom-left corner shows the top view of the integrated 3D plot, and the bottomright image is the corresponding experimental dI=dV map.
Direct Observation of Molecular Orbitals of Pentacene Physisorbed on Au(111) by Scanning Tunneling Microscope

June 2009

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1,158 Reads

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159 Citations

Physical Review Letters

Differential conductance (dI/dV) images taken with a low-temperature scanning tunneling microscope enabled the first observation of the electron probability distribution of the molecular orbitals of a pentacene molecule directly adsorbed on a metal surface. The three highest occupied molecular orbitals (HOMO, HOMO-1, and HOMO-2) and the lowest unoccupied molecular orbital are imaged. Thus dI/dV imaging without any intervening insulating layer permits the visualization of a large variety of molecular orbitals in the electronic cloud of a wide-gap molecule physisorbed on a metal surface.


Conformational dependence of tag induced intramolecular STM contrast in hexaphenylbenzene molecules

April 2009

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24 Reads

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6 Citations

Surface Science

Chemically tagged hexaphenylbenzene molecules physisorbed on Au(1 1 1) surface display their tag differently under STM as compared to their physisorption on a Cu(1 1 1) surface. Our STM findings complemented by First Principles and Quantum Chemistry calculations have attributed this difference to two different conformations adopted by these molecules on Au(1 1 1) in comparison to its one conformation on Cu(1 1 1). The demonstration of the sensitivity of the tag to its electronic or chemical environment would have important implications in designing single molecule machinery where the motion of the molecule is to be discerned by tracking its tag induced intramolecular STM contrast.


Citations (15)


... In 2020 [24], Soe et al introduced a novel tetrabenzophenazine molecule that effectively operated as a XORlike Boolean logic gate. Later in 2021 [25], the same group developed a digital full adder (3-input and 2-output) circuit using an aza-starphene molecule, implemented on a Au(111) surface. ...

Reference:

Multiple silicon dangling-bond charge qubits for quantum computing: a Hilbert-space analysis of the Hamiltonian
A Tetrabenzophenazine Low Voltage Single Molecule XOR Quantum Hamiltonian Logic Gate
  • Citing Article
  • March 2020

Chemical Physics Letters

... Over the past decades, the rapid developments of science and technology have allowed people to explore the quantum world. Research on quantum impurity systems (QIS) has become a significant subject and has received extensive attention for its widespread applications in physics [1,2] , chemistry [3][4][5][6] , nanoelectronics [7,8] , quantum information processing [9,10] , spintronics [11,12] , and quantum computation [13,14] . ...

On-Surface Atom by Atom Assembled Aluminium Bi-Nuclear Tetrabenzophenazine Organo-Metallic Magnetic Complex
  • Citing Article
  • December 2019

Nano Letters

... 40 Here, the BBD molecule must be manipulated with care not to open a conformation change path on its reduced state potential energy surface nor a chemical reaction path breaking some of its chemical bonds leading to the final destruction of the molecule since a molecule is often very unstable under high positive STM bias voltage pulses. 7,41 While exciting the BBD molecule at two different spatial locations of the same resonance maxima, the difference of mechanical response is a nice indication of how the electronic coupling between the tip apex and the electronic states of a molecule can give rise to different mechanical responses. Here and during an STM excitation (or imaging), the effective lateral extension of the tunneling electrons inelastic excitation is much narrower than the BBD molecular orbitals spatial lateral extension. ...

High Voltage STM Imaging of Single Copper Phthalocyanine
  • Citing Chapter
  • August 2013

... However, the nanoelectromechanical systems approach [40][41][42]. Simple mechanical structures fabrication method such as nano-gears is proposed for the fabrication and assembly of these nanodevice following this approach but is still at an early stage [43,44] ...

Nanogears Mechanics: From a Single Molecule to Solid-State Nanogears on a Surface

... Figure 10 depicts some recently reported large PA Hs that were synthesized under intramolecular oxidative coupling conditions.T etrabenzocircumpyrene derivatives 139 a-c have been synthesized in good yields using FeCl 3 as an oxidant in aCH 2 Cl 2 /CH 3 NO 2 mixture. [124] Compound 140 is an extended hexabenzocoronene that was obtained by Dichtel and co-workers. [125] Thea uthors observed that the formation of the first four bonds is very fast (Figure 10, blue bonds), thereby providing an isolable partly fused, twisted intermediate,w hich after prolonged exposure to the FeCl 3 oxidant furnishes the final HBC derivative in good yield. ...

Tetrabenzocircumpyrene: A Nanographene Fragment with an Embedded Peripentacene Core

Chemical Communications

... With the persistent and rapid development of STM manipulation, its application has been greatly extended from arranging the adsorbates in a desired manner to managing singlemolecule chemistry, such as inducing 1) intramolecular confor-mational changes; [15][16][17][18][19][20] 2) intermolecular covalent interactions by coupling two molecules in a controlled step-by-step way; [21] 3) single-molecule isomerization including cis-trans transition of azobenzene, [22][23][24] tautomerization of melamine, [25] isomerization of single chlorobenzene and its analogues, [26,27] and tautomerization of single free-base naphthalocyanine and porphycene molecules; [28,29] and 4) metal-organic complexes including metal-aromatic binding on single-crystal surfaces, [30][31][32] K atoms attaching to C 60 molecules, [33] hybrid magnetic complexes of V atoms and tetracyanoethylene ligands, [34] and metal-ligand interactions on insulating films. [35][36][37] Moreover, the dynamic behaviors of the adsorbates on surfaces could also be controlled by STM manipulations. ...

Manipulation of a single molecule ground state by means of gold atom contacts

Chemical Physics Letters

... of the channel, and the drain and source to have a greater influence, resulting in lower voltage and increased leakage. Therefore, digital circuit designers should consider adopting new technologies that overcome the challenges in COMS [1][2][3][4]. In chemistry, a dangling bond refers to an incomplete charge within an atom, and an atom with a dangling bond is called an immobile free radical. ...

Demonstration of a NOR logic gate using a single molecule and two surface gold atoms to encode the logical input

Physical review. B, Condensed matter

... Therefore, every four dimers on two adjacent rows easily form a stable structure, which is the well-known c(4×2) reconstruction. The c(4×2) reconstruction pattern was found to be dominant (50-60% at room temperature) and stable, consistent with the experiment by Manzano et al. [9]. Therefore, the Si(100)-c(4×2) surface is taken as the most appropriate and applicable research object for DA on the silicon surface. ...

Origin of the apparent (2× 1) topography of the Si (100)-c (4× 2) surface observed in low-temperature STM images
  • Citing Article
  • May 2011

Physical review. B, Condensed matter

... We speculate that splitting of LUMO states of tilted molecules arises from the breaking of intrinsic symmetry of picene molecules driven by the molecule-substrate interaction. 16,31 The dI/dV spectrum for the upright-standing molecules in the crystalline (001) monolayer is shown in Fig. 6(b). It is found that the HOMO and LUMO peaks appear at −2.3 eV and +2.5 eV, respectively. ...

Mapping the first electronic resonances of a Cu phthalocyanine STM tunnel junction
  • Citing Article
  • September 2012