Inductor¶

class
qucat.
L
(node_minus, node_plus, *args)[source]¶ A class representing an inductor
 Parameters
node_minus (integer) – Index corresponding to one node of inductor
node_minus – Index corresponding to the other node of the inductor
args (<float> or <str> or <float>,<str>) – Other arguments should be a float corresponding to the inductance, a string corresponding to the name of that value (ex: “L”), or both. If only a label is provided, a value for should be passed as a keyword argument in subsequent function calls (ex: L = 1e9) This is the best way to proceed if one wants to sweep the value of this inductor. Indeed, the most computationally expensive part of the analysis is performed upon initializing the circuit, subsequently changing the value of a component and recalculating a quantity such as the frequency or anharmonicity can be performed much faster.

zpf
(mode, quantity, **kwargs)¶ Returns contribution of a mode to the zeropoint fluctuations of a quantity for this component.
The quantity can be current (in units of Ampere), voltage (in Volts), charge (in electron charge), or flux (in units of the reduced flux quantum, \(\hbar/2e\)).
 Parameters
mode (integer) – Determine what mode to consider, where 0 designates the lowest frequency mode, and the others are arranged in order of increasing frequency
quantity (string) – One of ‘current’, ‘flux’, ‘charge’, ‘voltage’
kwargs – Values for unspecified circuit components, ex:
L=1e9
.
 Returns
contribution of the
mode
to the zeropoint fluctuations of thequantity
 Return type
Notes
This quantity is calculated by multiplying the voltage transfer function \(T_{rc}\) (between a reference component \(r\) and the annotated component \(c\) ), with \(X_{zpf,m,r}\), the zeropoint fluctuations of \(\hat{X}\) at the reference component.
Note that resistors make the transfer function \(T_{rc}\), and hence this quantity, complex.
For more detail on the underlying theory, see https://arxiv.org/pdf/1908.10342.pdf.