Gaussian Pulse

- General Form:
`gpulse([`*v1 v2 td pw per td1 td2*...] [*pattern_spec*])

- Examples:
`vsfq 0 0 gpulse(0 0 20p 2p 0 40p 60p)`

vpulse 1 0 gpulse(0 1 100p 5p 100p)

This generates a gaussian pulse signal, and as a special case, as a
voltage source will generate single flux quantum (SFQ) pulses. This
function applies only to transient analysis, where time is the running
variable. The following are the numerical parameters, the *pattern_spec* is used to specify a patterned pulse train and the
syntax is described in 2.15.3.5.

parameterdescriptiondefault valueunitsv1base value 0.0 volts or amps v2pulse peak value v1volts or amps tddelay time 0.0 seconds pwpulse width see description seconds perperiod 0.0 seconds

**Warning:** The pulse width is interpreted as the full-width
half-maximum in release 4.3.3 and later. In earlier releases, this
was taken as the ``variance'' (width where amplitude is 1/e of the
peak). Presently, this interpretation can be coerced by giving a **negative** pulse width, the absolute value will be used as the
variance.

The expression used to generate a pulse is
*pw* > 0
:

value=v1 + (v2 -v1)^{ . }exp(- (4^{ . }ln(2)^{ . }(time-td)/pw)^{2})

value=v1 + (v2 -v1)^{ . }exp(- ((time-td)/ -pw)^{2})

The *td* delay value specifies the time of the initial pulse peak.
The *pw* defines the pulse width, as described above. If the *per* is given a nonzero value larger than twice the *pw*, a train
of pulses will be generated, the first being at *td* and at time
increments of *per* thereafter.

Numbers found after the *per* are taken as additional delays,
similar to *td*. The output is a superposition of pulses found
at each delay value (including *td*). If the *per* is given
a value 0.0, only one pulse per delay value is emitted. If the *per* specifies a viable period, pulses are emitted at each delay value
and increments of *per*.

Periodic pulses can be set to a pattern via the *pattern_spec*,
which can appear following all delay values, if any. The syntax is
described in 2.15.3.5.

A single flux quantum (SFQ) pulse, as a voltage applied across an inductor, will induce a single flux quantum of

=whereh/(2e) = 2.06783fWb

If the `pw` is not given or given as zero, the source will be
configured to produce an SFQ pulse with the given amplitude. Thus,
the actual pulse width will be computed internally, with amplitude not
zero, as

where is the flux quantum whose value is given above.pw= 2/(abs(v2 -v1))

Similarly, if the amplitude is set to zero, i.e., *v2* = *v1*, the amplitude will be computed from the pulse width to yield an
SFQ pulse. The computed amplitude is

v2 =v1 + 2/(pw)

If both amplitude and pulse width are set to zero or not given, the full-width half-maximum SFQ pulse width is taken as the TSTEP transient analysis parameter, and the amplitude is computed as above.

In superconducting electronics, single flux quantum pulses are generated and received by logic circuits. A generator of SFQ pulses is therefor a useful item when working with this technology.

Example

* gaussian pulse

v1 1 0 gpulse(0 0 20p 2p 0 40p)

l1 1 2 10p

b1 2 0 100 jj3 area=.2

r2 2 0 2

.tran .1p 100p uic

.plot tran v(1) v(2) i(l1) ysep

* Nb 4500 A/cm2

.model jj3 jj(rtype=1, cct=1, icon=10m, vg=2.8m, delv=0.08m,

+ icrit=1m, r0=30, rn=1.7, cap=1.31p)

In the example, the generator produces two SFQ pulses. The second pulse causes the Josephson junction to emit a flux quantum, the second one from the source is therefor expelled. The inductor current shows the same value before and after the second pulse, as expected.