本文整理汇总了Python中taref.plotter.api.Plotter.set_ylim方法的典型用法代码示例。如果您正苦于以下问题：Python Plotter.set_ylim方法的具体用法？Python Plotter.set_ylim怎么用？Python Plotter.set_ylim使用的例子？那么恭喜您, 这里精选的方法代码示例或许可以为您提供帮助。您也可以进一步了解该方法所在类taref.plotter.api.Plotter的用法示例。
在下文中一共展示了Plotter.set_ylim方法的7个代码示例，这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞，您的评价将有助于系统推荐出更棒的Python代码示例。
示例1: anton_lamb_shift_plot
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def anton_lamb_shift_plot(fig_width=9.0, fig_height=6.0):
"""reproduces coupling/lamb shift plot in Anton's paper"""
pl=Plotter(fig_width=fig_width, fig_height=fig_height)
EjdivEc=linspace(0.1, 300, 10000)
Ej=EjdivEc*antonqdt.Ec
#E0, E1, E2=antonqdt._get_transmon_energy_levels(Ej=Ej, n_energy=3)
fq=antonqdt._get_fq(Ej)
#anharm=(E2-E1)-(E1-E0)
#E0p, E1p, E2p=antonqdt._get_lamb_shifted_transmon_energy_levels(Ej=Ej, n_energy=3)
#anharmp=(E2p-E1p)-(E1p-E0p)
#fq= (E1-E0)/h#qdt.call_func("fq", Ej=EjdivEc*qdt.Ec)
coup=antonqdt._get_coupling(fq)
ls=antonqdt._get_Lamb_shift(fq)
line(fq/antonqdt.f0, 2.0*coup/(2.0*antonqdt.max_coupling), plotter=pl, linewidth=0.5, color="red", label=r"$\Gamma$, $N=10$")
line(fq/antonqdt.f0, ls/(2.0*antonqdt.max_coupling), plotter=pl, color="green", linewidth=0.5, label=r"$\Delta$, $N=10$")
#antonqdt.Np=3
Ej=EjdivEc*antonqdt3.Ec
fq=antonqdt3._get_fq(Ej)
coup=antonqdt3._get_coupling(fq)
ls=antonqdt3._get_Lamb_shift(fq)
line(fq/antonqdt3.f0, 2.0*coup/(2.0*antonqdt3.max_coupling), plotter=pl, linewidth=0.5, color="blue", label=r"$\Gamma$, $N=3$")
line(fq/antonqdt3.f0, ls/(2.0*antonqdt3.max_coupling), plotter=pl, color="black", linewidth=0.5, label=r"$\Delta$, $N=3$")
pl.set_ylim(-0.4, 1.0)
pl.set_xlim(0.2, 1.8)
pl.xlabel=r"$f_{10}/f_{IDT}$"
pl.ylabel=r"$\Delta/\Gamma_{10}^{MAX}$"
pl.legend(loc='upper right')
return pl示例2: magabs_colormesh
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def magabs_colormesh(self):
pl=Plotter(fig_width=9.0, fig_height=6.0, name="magabs_{}".format(self.name))
pl, pf=colormesh(self.frequency/1e9, self.yoko, (self.MagdB.transpose()-self.MagdB[:, 0]), plotter=pl)
pf.set_clim(-0.3, 0.1)
pl.set_xlim(min(self.frequency/1e9), max(self.frequency/1e9))
pl.set_ylim(min(self.yoko), max(self.yoko))
pl.ylabel="Yoko (V)"
pl.xlabel="Frequency (GHz)"
return pl示例3: magabs_colormesh2
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def magabs_colormesh2(self, f0=5.35e9, alpha=0.45, pl=None):
fq_vec=array([sqrt(f*(f-2*qdt.call_func("Lamb_shift", f=f, f0=f0, couple_mult=alpha))) for f in self.frequency])
pl=Plotter(fig_width=9.0, fig_height=6.0, name="magabs_{}".format(self.name))
pl, pf=colormesh(self.yoko, fq_vec/1e9, (self.MagdB.transpose()-self.MagdB[:, 0]).transpose(), plotter=pl)
pf.set_clim(-0.3, 0.1)
pl.set_ylim(min(fq_vec/1e9), max(fq_vec/1e9))
pl.set_xlim(min(self.yoko), max(self.yoko))
pl.ylabel="Yoko (V)"
pl.xlabel="Frequency (GHz)"
return pl示例4: magabs_colormesh2
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def magabs_colormesh2(self, offset=-0.08, flux_factor=0.52, Ejmax=h*44.0e9, f0=5.35e9, alpha=0.7, pl=None):
fq_vec=array([sqrt(f*(f+alpha*calc_freq_shift(f, qdt.ft, qdt.Np, f0, qdt.epsinf, qdt.W, qdt.Dvv))) for f in self.frequency])
pl=Plotter(fig_width=9.0, fig_height=6.0, name="magabs_{}".format(self.name))
pl, pf=colormesh(fq_vec, self.yoko, (self.MagdB.transpose()-self.MagdB[:, 0]), plotter=pl)
pf.set_clim(-0.3, 0.1)
#pl.set_xlim(min(self.frequency/1e9), max(self.frequency/1e9))
pl.set_ylim(min(self.yoko), max(self.yoko))
pl.ylabel="Yoko (V)"
pl.xlabel="Frequency (GHz)"
return pl示例5: anharm_plot
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def anharm_plot(qdt, fig_width=9.0, fig_height=6.0, ymin=-1.5, ymax=1.0):
"""Lamb shifted anharmonicity plot"""
pl=Plotter(fig_width=fig_width, fig_height=fig_height)
EjdivEc=linspace(0.1, 300, 3000)
Ej=EjdivEc*qdt.Ec
E0, E1, E2=qdt._get_transmon_energy_levels(Ej=Ej, n_energy=3)
anharm=(E2-E1)-(E1-E0)
E0p, E1p, E2p=qdt._get_lamb_shifted_transmon_energy_levels(Ej=Ej, n_energy=3)
anharmp=(E2p-E1p)-(E1p-E0p)
fq= (E1-E0)/h
ls_fq=(E1p-E0p)/h
fq2=(E2-E1)/h
ls_fq2=(E2p-E1p)/h
line(EjdivEc, anharm/h/1e9, plotter=pl, linewidth=0.5, color="purple", label=r"anharm")
line(EjdivEc, anharmp/h/1e9, plotter=pl, linewidth=0.5, color="black", label=r"ls anharm")
line(EjdivEc, (ls_fq-fq)/1e9, plotter=pl, color="blue", linewidth=0.5, label=r"$\Delta_{1,0}$")
line(EjdivEc, (ls_fq2-fq2)/1e9, plotter=pl, color="red", linewidth=0.5, label=r"$\Delta_{2,1}$")
pl.set_ylim(ymin, ymax)
#pl.set_xlim(0.7, 1.3)
pl.xlabel=r"$E_J/E_C$"
pl.ylabel=r"$\Delta$ (GHz)"
pl.legend(loc='lower left')
#pl.set_ylim(-2, 1.5)
#pl.set_xlim(0.0, 70)
#anharm=qdt.call_func("anharm", EjdivEc=EjdivEc)
#anharmp=qdt.call_func("lamb_shifted_anharm", EjdivEc=EjdivEc)
#fq=qdt.call_func("fq", Ej=EjdivEc*qdt.Ec)
#ls_fq=qdt.call_func("lamb_shifted_fq", EjdivEc=EjdivEc)
#ls_fq2=qdt.call_func("lamb_shifted_fq2", EjdivEc=EjdivEc)
#pl, pf=line(fq, anharm/h, linewidth=0.5, color="black", label=r"$\Delta_{2,1}-\Delta_{1,0}$")
#pl, pf=line(EjdivEc, anharmp/h/1e9, linewidth=1.0, color="black", label=r"$\Delta_{2,1}-\Delta_{1,0}$", plotter=pl)
#line(EjdivEc, anharm/h/1e9, linewidth=1.0, color="purple", label=r"anharm", plotter=pl)
#line(EjdivEc, (ls_fq-fq)/1e9, plotter=pl, color="blue", linewidth=1.0, label=r"$\Delta_{1,0}$")
#E0, E1, E2=qdt.call_func("transmon_energy_levels", EjdivEc=EjdivEc, n_energy=3)
#fq2=(E2-E1)/h
#line(EjdivEc, (ls_fq2-fq2)/1e9, plotter=pl, color="red", linewidth=1.0, label=r"$\Delta_{2,1}$")
#pl.xlabel=r"$E_j/E_c$"
#pl.ylabel=r"$\Delta (GHz)$"
#pl.legend(loc='lower right')
#fq=qdt.call_func("lamb_shifted_fq", EjdivEc=EjdivEc)
#line(EjdivEc, fq, plotter=pl, color="green", linewidth=0.5)
#line(EjdivEc, E1p, plotter=pl, color="green", linewidth=0.5)
#line(EjdivEc, E2p, plotter=pl, color="purple", linewidth=0.5)
return pl示例6: anton_anharm_plot
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def anton_anharm_plot(fig_width=9, fig_height=6):
"""reproduces anharm plot in Anton's paper"""
pl=Plotter(fig_width=fig_width, fig_height=fig_height)
#print qdt.f0*h/qdt.Ec, qdt.epsinf/3.72
#qdt.Np=10
#qdt.Ec=qdt.f0*0.1*h
EjdivEc=linspace(0.1, 300, 3000)
Ej=EjdivEc*antonqdt.Ec
print antonqdt.C, antonqdt.C, antonqdt.Ec, antonqdt._get_Ec(antonqdt.C)
print antonqdt.max_coupling, antonqdt.epsinf, antonqdt.f0*h/antonqdt.Ec
E0, E1, E2=antonqdt._get_transmon_energy_levels(Ej=Ej, n_energy=3)
anharm=(E2-E1)-(E1-E0)
E0p, E1p, E2p=antonqdt._get_lamb_shifted_transmon_energy_levels(Ej=Ej, n_energy=3)
anharmp=(E2p-E1p)-(E1p-E0p)
fq= (E1-E0)/h#qdt.call_func("fq", Ej=EjdivEc*qdt.Ec)
ls_fq=(E1p-E0p)/h #qdt.call_func("lamb_shifted_fq", EjdivEc=EjdivEc)
fq2=(E2-E1)/h
ls_fq2=(E2p-E1p)/h #qdt.call_func("lamb_shifted_fq2", EjdivEc=EjdivEc)
line(fq/antonqdt.f0, (anharmp/h-anharm/h)/(2.0*antonqdt.max_coupling), plotter=pl, linewidth=0.5, color="black", label=r"$\Delta_{2,1}-\Delta_{1,0}$")
line(fq/antonqdt.f0, (ls_fq-fq)/(2.0*antonqdt.max_coupling), plotter=pl, color="blue", linewidth=0.5, label=r"$\Delta_{1,0}$")
line(fq/antonqdt.f0, (ls_fq2-fq2)/(2.0*antonqdt.max_coupling), plotter=pl, color="red", linewidth=0.5, label=r"$\Delta_{2,1}$")
pl.set_ylim(-1.0, 0.6)
pl.set_xlim(0.7, 1.3)
pl.xlabel=r"$f_{10}/f_{IDT}$"
pl.ylabel=r"$\Delta/\Gamma_{10}^{MAX}$"
pl.legend(loc='lower left')
#fq=qdt.call_func("lamb_shifted_fq", EjdivEc=EjdivEc)
#line(EjdivEc, fq, plotter=pl, color="green", linewidth=0.5)
#line(EjdivEc, E1p, plotter=pl, color="green", linewidth=0.5)
#line(EjdivEc, E2p, plotter=pl, color="purple", linewidth=0.5)
return pl示例7: anharm_plot2
# 需要导入模块: from taref.plotter.api import Plotter [as 别名]
# 或者: from taref.plotter.api.Plotter import set_ylim [as 别名]
def anharm_plot2():
"""reproduces anharm plot in Anton's paper"""
set_tag(qdt, "EjdivEc", log=False)
set_tag(qdt, "Ej", log=False)
pl=Plotter(fig_width=9.0, fig_height=6.0)
#qdt.epsinf=qdt.epsinf/3.72
#qdt.Np=10
#qdt.Ec=qdt.fq*0.1*h
print qdt.max_coupling, qdt.coupling_approx
#flux_o_flux0=qdt.call_func("flux_over_flux0", voltage=yoko)
#Ej=qdt.call_func("Ej", flux_over_flux0=flux_o_flux0)
#EjdivEc=Ej/qdt.Ec
anharm=qdt.call_func("anharm", EjdivEc=EjdivEc)
anharmp=qdt.call_func("lamb_shifted_anharm", EjdivEc=EjdivEc)
fq=qdt.call_func("fq", Ej=EjdivEc*qdt.Ec)
ls_fq=qdt.call_func("lamb_shifted_fq", EjdivEc=EjdivEc)
ls_fq2=qdt.call_func("lamb_shifted_fq2", EjdivEc=EjdivEc)
#pl, pf=line(fq, anharm/h, linewidth=0.5, color="black", label=r"$\Delta_{2,1}-\Delta_{1,0}$")
pl, pf=line(EjdivEc, anharmp/h/1e9, linewidth=1.0, color="black", label=r"$\Delta_{2,1}-\Delta_{1,0}$", plotter=pl)
line(EjdivEc, anharm/h/1e9, linewidth=1.0, color="purple", label=r"anharm", plotter=pl)
line(EjdivEc, (ls_fq-fq)/1e9, plotter=pl, color="blue", linewidth=1.0, label=r"$\Delta_{1,0}$")
E0, E1, E2=qdt.call_func("transmon_energy_levels", EjdivEc=EjdivEc, n_energy=3)
fq2=(E2-E1)/h
line(EjdivEc, (ls_fq2-fq2)/1e9, plotter=pl, color="red", linewidth=1.0, label=r"$\Delta_{2,1}$")
pl.set_ylim(-2, 1.5)
#pl.set_xlim(0.0, 70)
pl.xlabel=r"$E_j/E_c$"
pl.ylabel=r"$\Delta (GHz)$"
#pl.legend(loc='lower right')
#fq=qdt.call_func("lamb_shifted_fq", EjdivEc=EjdivEc)
#line(EjdivEc, fq, plotter=pl, color="green", linewidth=0.5)
#line(EjdivEc, E1p, plotter=pl, color="green", linewidth=0.5)
#line(EjdivEc, E2p, plotter=pl, color="purple", linewidth=0.5)
return pl