18 research outputs found
A Hessian-Free Method to Prevent Zero-Point Energy Leakage in Classical Trajectories
The
problem associated with the zero-point energy (ZPE) leak in
classical trajectory calculations is well known. Since ZPE is a manifestation
of the quantum uncertainty principle, there are no restrictions on
energy during the classical propagation of nuclei. This phenomenon
can lead to unphysical results, such as forming products without the
ZPE in the internal vibrational degrees of freedom (DOFs). The ZPE
leakage also permits reactions below the quantum threshold for the
reaction. We have developed a new Hessian-free method, inspired by
the Lowe-Andersen thermostat model, to prevent energy dipping below
a threshold in the local-pair (LP) vibrational DOFs. The idea is to
pump the leaked energy to the corresponding local vibrational mode
taken from the other vibrational DOFs. We have applied the new correction
protocol on the ab-initio ground-state molecular dynamics simulation
of the water dimer (H2O)2, which dissociates
due to unphysical ZPE spilling from high-frequency OH modes. The LP-ZPE
method has been able to prevent the ZPE spilling of the OH stretching
modes by pumping back the leaked energy into the corresponding modes,
while this energy is taken from the other modes of the dimer itself,
keeping the system as a microcanonical ensemble
pH-Sensitive Nanoaggregates for Site-Specific Drug-Delivery as Well as Cancer Cell Imaging
Multifunctional
polymeric nanoaggregates could enable targeted cancer therapy and
imaging, which eventually facilitate monitoring of the therapeutic
effect. A fluorescent nanoaggregate is constructed for theranostic
application. Chlorambucil (Chl), a fluorescent inactive chemotherapeutic
agent, is covalently attached to the nanoaggregate for therapeutic
action. The pyrene (Py) motif is also covalently attached to the nanoaggregates,
with the motivation of cancer cell imaging. This nanoaggregate is
further functionalized with biotin (Btn) for receptor-mediated drug
delivery. The efficiency of this system is evaluated by in vitro cell
studies to prove its receptor-mediated internalization as well as
theranostic capabilities. This newly designed nanocarrier, Nor–Chl–Py–Btn
(Nor, norbornene), has the ability to combine both therapeutic and
diagnostic capabilities into a single polymer that offers existing
prospects for the development of nanomedicine
pH-Sensitive Nanoaggregates for Site-Specific Drug-Delivery as Well as Cancer Cell Imaging
Multifunctional
polymeric nanoaggregates could enable targeted cancer therapy and
imaging, which eventually facilitate monitoring of the therapeutic
effect. A fluorescent nanoaggregate is constructed for theranostic
application. Chlorambucil (Chl), a fluorescent inactive chemotherapeutic
agent, is covalently attached to the nanoaggregate for therapeutic
action. The pyrene (Py) motif is also covalently attached to the nanoaggregates,
with the motivation of cancer cell imaging. This nanoaggregate is
further functionalized with biotin (Btn) for receptor-mediated drug
delivery. The efficiency of this system is evaluated by in vitro cell
studies to prove its receptor-mediated internalization as well as
theranostic capabilities. This newly designed nanocarrier, Nor–Chl–Py–Btn
(Nor, norbornene), has the ability to combine both therapeutic and
diagnostic capabilities into a single polymer that offers existing
prospects for the development of nanomedicine
pH-Sensitive Nanoaggregates for Site-Specific Drug-Delivery as Well as Cancer Cell Imaging
Multifunctional
polymeric nanoaggregates could enable targeted cancer therapy and
imaging, which eventually facilitate monitoring of the therapeutic
effect. A fluorescent nanoaggregate is constructed for theranostic
application. Chlorambucil (Chl), a fluorescent inactive chemotherapeutic
agent, is covalently attached to the nanoaggregate for therapeutic
action. The pyrene (Py) motif is also covalently attached to the nanoaggregates,
with the motivation of cancer cell imaging. This nanoaggregate is
further functionalized with biotin (Btn) for receptor-mediated drug
delivery. The efficiency of this system is evaluated by in vitro cell
studies to prove its receptor-mediated internalization as well as
theranostic capabilities. This newly designed nanocarrier, Nor–Chl–Py–Btn
(Nor, norbornene), has the ability to combine both therapeutic and
diagnostic capabilities into a single polymer that offers existing
prospects for the development of nanomedicine
pH-Sensitive Nanoaggregates for Site-Specific Drug-Delivery as Well as Cancer Cell Imaging
Multifunctional
polymeric nanoaggregates could enable targeted cancer therapy and
imaging, which eventually facilitate monitoring of the therapeutic
effect. A fluorescent nanoaggregate is constructed for theranostic
application. Chlorambucil (Chl), a fluorescent inactive chemotherapeutic
agent, is covalently attached to the nanoaggregate for therapeutic
action. The pyrene (Py) motif is also covalently attached to the nanoaggregates,
with the motivation of cancer cell imaging. This nanoaggregate is
further functionalized with biotin (Btn) for receptor-mediated drug
delivery. The efficiency of this system is evaluated by in vitro cell
studies to prove its receptor-mediated internalization as well as
theranostic capabilities. This newly designed nanocarrier, Nor–Chl–Py–Btn
(Nor, norbornene), has the ability to combine both therapeutic and
diagnostic capabilities into a single polymer that offers existing
prospects for the development of nanomedicine
ADT: A Generalized Algorithm and Program for Beyond Born–Oppenheimer Equations of “<i>N</i>” Dimensional Sub-Hilbert Space
The
major bottleneck of first principle based beyond Born–Oppenheimer
(BBO) treatment originates from large number and complicated expressions
of adiabatic to diabatic transformation (ADT) equations for higher
dimensional sub-Hilbert spaces. In order to overcome such shortcoming,
we develop a generalized algorithm, “ADT” to generate
the nonadiabatic equations through symbolic manipulation and to construct
highly accurate diabatic surfaces for molecular processes involving
excited electronic states. It is noteworthy to mention that the nonadiabatic
coupling terms (NACTs) often become singular (removable) at degenerate
point(s) or along a seam in the nuclear configuration space (CS) and
thereby, a unitary transformation is required to convert the kinetically
coupled (adiabatic) Hamiltonian to a potentially (diabatic) one to
avoid such singularity(ies). The “ADT” program can be
efficiently used to (a) formulate analytic functional forms of differential
equations for ADT angles and diabatic potential energy matrix and
(b) solve the set of coupled differential equations numerically to
evaluate ADT angles, residue due to singularity(ies), ADT matrices,
and finally, diabatic potential energy surfaces (PESs). For the numerical
case, user can directly provide ab initio data (adiabatic
PESs and NACTs) as input files to this software or can generate those
input files through in-built python codes interfacing MOLPRO followed
by ADT calculation. In order to establish the workability of our program
package, we selectively choose six realistic molecular species, namely,
NO2 radical, H3+, F + H2, NO3 radical, C6H6+ radical
cation, and 1,3,5-C6H3F3+ radical cation, where two, three, five and six electronic states
exhibit profound nonadiabatic interactions and are employed to compute
diabatic PESs by using ab initio calculated adiabatic
PESs and NACTs. The “ADT” package released under the
GNU General Public License v3.0 (GPLv3) is available at https://github.com/AdhikariLAB/ADT-Program and also as the Supporting Information of this article
Construction of Diabatic Hamiltonian Matrix from ab Initio Calculated Molecular Symmetry Adapted Nonadiabatic Coupling Terms and Nuclear Dynamics for the Excited States of Na<sub>3</sub> Cluster
We present the molecular symmetry
(MS) adapted treatment of nonadiabatic
coupling terms (NACTs) for the excited electronic states (2<sup>2</sup>E′ and 1<sup>2</sup>A<sub>1</sub><sup>′</sup>) of Na<sub>3</sub> cluster, where the
adiabatic potential energy surfaces (PESs) and the NACTs are calculated
at the MRCI level by using an ab initio quantum chemistry package
(MOLPRO). The signs of the NACTs at each point of the configuration
space (CS) are determined by employing appropriate irreducible representations
(IREPs) arising due to MS group, and such terms are incorporated into
the adiabatic to diabatic transformation (ADT) equations to obtain
the ADT angles. Since those sign corrected NACTs and the corresponding
ADT angles demonstrate the validity of curl condition for the existence
of three-state (2<sup>2</sup>E′ and 1<sup>2</sup>A<sub>1</sub><sup>′</sup>) sub-Hilbert
space, it becomes possible to construct the continuous, single-valued,
symmetric, and smooth 3 × 3 diabatic Hamiltonian matrix. Finally,
nuclear dynamics has been carried out on such diabatic surfaces to
explore whether our MS-based treatment of diabatization can reproduce
the pattern of the experimental spectrum for system <b>B</b> of Na<sub>3</sub> cluster
ADT: A Generalized Algorithm and Program for Beyond Born–Oppenheimer Equations of “<i>N</i>” Dimensional Sub-Hilbert Space
The
major bottleneck of first principle based beyond Born–Oppenheimer
(BBO) treatment originates from large number and complicated expressions
of adiabatic to diabatic transformation (ADT) equations for higher
dimensional sub-Hilbert spaces. In order to overcome such shortcoming,
we develop a generalized algorithm, “ADT” to generate
the nonadiabatic equations through symbolic manipulation and to construct
highly accurate diabatic surfaces for molecular processes involving
excited electronic states. It is noteworthy to mention that the nonadiabatic
coupling terms (NACTs) often become singular (removable) at degenerate
point(s) or along a seam in the nuclear configuration space (CS) and
thereby, a unitary transformation is required to convert the kinetically
coupled (adiabatic) Hamiltonian to a potentially (diabatic) one to
avoid such singularity(ies). The “ADT” program can be
efficiently used to (a) formulate analytic functional forms of differential
equations for ADT angles and diabatic potential energy matrix and
(b) solve the set of coupled differential equations numerically to
evaluate ADT angles, residue due to singularity(ies), ADT matrices,
and finally, diabatic potential energy surfaces (PESs). For the numerical
case, user can directly provide ab initio data (adiabatic
PESs and NACTs) as input files to this software or can generate those
input files through in-built python codes interfacing MOLPRO followed
by ADT calculation. In order to establish the workability of our program
package, we selectively choose six realistic molecular species, namely,
NO2 radical, H3+, F + H2, NO3 radical, C6H6+ radical
cation, and 1,3,5-C6H3F3+ radical cation, where two, three, five and six electronic states
exhibit profound nonadiabatic interactions and are employed to compute
diabatic PESs by using ab initio calculated adiabatic
PESs and NACTs. The “ADT” package released under the
GNU General Public License v3.0 (GPLv3) is available at https://github.com/AdhikariLAB/ADT-Program and also as the Supporting Information of this article
Recommendations for Velocity Adjustment in Surface Hopping
This
study investigates velocity adjustment directions after hopping
in surface hopping dynamics. Using fulvene and a protonated Schiff
base (PSB4) as case studies, we investigate the population decay and
reaction yields of different sets of dynamics with the velocity adjusted
in either the nonadiabatic coupling, gradient difference, or momentum
directions. For the latter, in addition to the conventional algorithm,
we investigated the performance of a reduced kinetic energy reservoir
approach recently proposed. Our evaluation also considered velocity
adjustment in the directions of approximate nonadiabatic coupling
vectors. While results for fulvene are susceptible to the adjustment
approach, PSB4 is not. We correlated this dependence to the topography
near the conical intersections. When nonadiabatic coupling vectors
are unavailable, the gradient difference direction is the best adjustment
option. If the gradient difference is also unavailable, a semiempirical
vector direction or the momentum direction with a reduced kinetic
energy reservoir becomes an excellent option to prevent an artificial
excess of back hoppings. The precise velocity adjustment direction
is less crucial for describing the nonadiabatic dynamics than the
kinetic energy reservoir’s size
Site-Specific Amphiphilic Magnetic Copolymer Nanoaggregates for Dual Imaging
Molecular
imaging along with combinations of imaging modalities
can provide a thorough understanding of disease, in particular, tumors.
Magnetic resonance imaging (MRI) offers exceptional tissue contrast
and resolution; whereas optical imaging provides high sensitivity.
Hence a norbornene based copolymer (<b>Nor-Cob-Py-Fol</b>) is
reported in this paper as a dual-imaging agent. <b>Nor-Cob-Py-Fol</b> having Co<sup>2+</sup> complex, pyrene and poly(ethylene glycol)
derived folate, have been synthesized using ring-opening metathesis
polymerization (<b>ROMP</b>). All the monomers and polymers
are characterized by <sup>1</sup>H NMR, IR, GPC, and TGA techniques.
The morphology of the copolymer nanoaggregates has been evaluated
with DLS, TEM, and SEM techniques. The functionalization of Co<sup>2+</sup> to the polymer is monitored by FTIR, <sup>1</sup>H NMR,
and <sup>13</sup>C NMR spectroscopy. Furthermore, the presence of
Co<sup>2+</sup> in the nanoaggregates is confirmed by the EDX (SEM)
technique. To prove the MRI capabilities nature of copolymer nanoaggregates,
NMR experiment is performed at room temperature. Cell viability studies
suggest the biocompatibility nature of the copolymer. Flow cytometry
as well as epifluoroscence microscope experiments clearly demonstrate
the dual-imaging ability of the newly designed copolymer. The much
higher relaxivity ratio (<i>r</i><sub>2</sub>/<i>r</i><sub>1</sub>) of the present method clearly establishes the superiority
of our system as one of the best contrast agents known to the practitioners
of magnetic resonance imaging
