Operator File Interpretation¶
The previous chapters introduced the mathematical form of the vibronic Hamiltonian and showed how the vibrational, electronic, linear, and quadratic coupling terms are combined to describe the coupled electron-nuclear dynamics.
In practice, however, MCTDH does not read these equations directly. Instead, the Hamiltonian is written using the operator-file syntax, where every keyword represents a mathematical operator or parameter. Understanding this correspondence makes it much easier to interpret, modify, and debug operator files.
This section summarizes the relationship between the mathematical Hamiltonian and the generated MCTDH operator file.
Overall Structure¶
Every generated operator file consists of three main parts.
The first section provides descriptive information about the calculation, the second defines all numerical parameters, and the third constructs the Hamiltonian using those parameters.
Vibrational Parameters¶
The vibrational frequencies appear in the parameter section as
where
is the harmonic frequency of the \(i^{\text{th}}\) active normal mode.
These frequencies are obtained from the harmonic vibrational analysis and determine the kinetic and potential energy operators for each mode.
Electronic Parameters¶
The diagonal electronic energies are written as
representing
The off-diagonal parameters
represent the electronic coupling matrix elements
These quantities are extracted directly from the diabatic electronic structure calculations.
Linear Coupling Parameters¶
Linear vibronic coupling constants are represented by
This notation can be interpreted as
| Symbol | Meaning |
|---|---|
h |
Hamiltonian parameter |
12 |
Coupling between electronic states 1 and 2 |
k |
Linear vibronic coupling |
5 |
Vibrational mode 5 |
Mathematically,
When used inside the Hamiltonian,
it represents
Quadratic Coupling Parameters¶
Quadratic coupling parameters use the notation
where
| Symbol | Meaning |
|---|---|
h |
Hamiltonian parameter |
12 |
Coupled electronic states |
g |
Quadratic vibronic coupling |
5 |
Vibrational mode |
which corresponds to
Within the Hamiltonian,
represents
The factor of one-half arises from the second-order Taylor expansion of the electronic Hamiltonian.
Coordinate Operators¶
The Hamiltonian section contains several operator keywords.
| Operator | Mathematical Meaning |
|---|---|
KE |
\( -\frac12\dfrac{\partial^2}{\partial Q^2} \) |
q |
\(Q\) |
q^2 |
\(Q^2\) |
Thus,
represents
while
represents
Electronic Operators¶
Electronic operators specify which electronic states are connected by a Hamiltonian term.
Examples include
Their mathematical interpretation is
S1&1→ \(|1\rangle\!\langle1|\)S2&2→ \(|2\rangle\!\langle2|\)S1&2→ \(|1\rangle\!\langle2|\)S2&3→ \(|2\rangle\!\langle3|\)
Diagonal operators contribute to the electronic energies, while off-diagonal operators describe transitions between electronic states.
Reading a Hamiltonian Line¶
Consider the operator-file entry
This line can be interpreted as
h12_k7— linear coupling constant,|7 q— normal coordinate of mode 7,|el S1&2— interaction between electronic states 1 and 2.
The corresponding mathematical expression is
Similarly,
represents
Complete Mapping¶
The table below summarizes the correspondence between the operator-file syntax and the mathematical Hamiltonian.
| Operator File | Mathematical Quantity | Physical Meaning |
|---|---|---|
w1 |
\(\omega_1\) | Vibrational frequency |
KE |
\( -\frac12\partial^2/\partial Q^2 \) | Kinetic energy |
q |
\(Q\) | Normal coordinate |
q^2 |
\(Q^2\) | Harmonic coordinate |
e11 |
\(E_1\) | Diabatic state energy |
e12 |
\(V_{12}\) | Electronic coupling |
h11_k1 |
\(k_{11}^{(1)}\) | Linear intrastate coupling |
h12_k1 |
\(k_{12}^{(1)}\) | Linear interstate coupling |
h11_g1 |
\(g_{11}^{(1)}\) | Quadratic intrastate coupling |
h12_g1 |
\(g_{12}^{(1)}\) | Quadratic interstate coupling |
S1&2 |
( | 1\rangle\langle2 |
Summary¶
Every line in an MCTDH operator file represents a specific term in the vibronic Hamiltonian. The parameter section defines the numerical values of the vibrational frequencies, electronic energies, and vibronic coupling constants, while the Hamiltonian section combines these quantities with the vibrational and electronic operators to construct the complete Hamiltonian. Understanding this correspondence provides a direct link between the mathematical formulation of the vibronic Hamiltonian and its implementation within MCTDH, making it easier to interpret, validate, and modify operator files for quantum dynamics calculations.