Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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46586 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ | 0.6911 | 0.8637 | 0.8002 | [M:[0.9807, 0.9807, 1.1197, 0.6795, 0.6795], q:[0.5791, 0.4402], qb:[0.4402, 0.7799], phi:[0.4402]] | [M:[[1, -7], [-1, -11], [0, 4], [-2, 2], [2, 10]], q:[[0, 11], [-1, -4]], qb:[[1, 0], [0, 1]], phi:[[0, -2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}^{2}$ | ${}M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | -2 | 2*t^2.039 + t^2.641 + 2*t^2.942 + t^3.359 + 2*t^3.66 + t^3.961 + 4*t^4.077 + 2*t^4.378 + 2*t^4.68 + t^4.795 + 4*t^4.981 + t^5.282 + 2*t^5.398 + 4*t^5.699 + 3*t^5.884 - 2*t^6. + 6*t^6.116 + 2*t^6.301 + 2*t^6.417 + 4*t^6.602 + 3*t^6.718 + 2*t^6.834 + 8*t^7.019 + 3*t^7.32 + 4*t^7.436 + 8*t^7.737 + 7*t^7.923 - 4*t^8.039 + 9*t^8.154 + 2*t^8.34 + 4*t^8.455 + 4*t^8.641 + 4*t^8.757 + 4*t^8.826 + 4*t^8.872 - 8*t^8.942 - t^4.32/y - (2*t^6.359)/y + t^7.077/y - (2*t^7.263)/y + (2*t^7.378)/y + (2*t^7.68)/y + (4*t^7.981)/y + (2*t^8.282)/y - t^8.398/y + (2*t^8.583)/y + (4*t^8.699)/y + t^8.884/y - t^4.32*y - 2*t^6.359*y + t^7.077*y - 2*t^7.263*y + 2*t^7.378*y + 2*t^7.68*y + 4*t^7.981*y + 2*t^8.282*y - t^8.398*y + 2*t^8.583*y + 4*t^8.699*y + t^8.884*y | (g2^2*t^2.039)/g1^2 + g1^2*g2^10*t^2.039 + t^2.641/g2^4 + t^2.942/(g1*g2^11) + (g1*t^2.942)/g2^7 + g2^4*t^3.359 + t^3.66/(g1*g2^3) + g1*g2*t^3.66 + t^3.961/g2^6 + (g2^4*t^4.077)/g1^4 + 2*g2^12*t^4.077 + g1^4*g2^20*t^4.077 + (g2^5*t^4.378)/g1 + g1*g2^9*t^4.378 + t^4.68/(g1^2*g2^2) + g1^2*g2^6*t^4.68 + g2^20*t^4.795 + t^4.981/(g1^3*g2^9) + t^4.981/(g1*g2^5) + (g1*t^4.981)/g2 + g1^3*g2^3*t^4.981 + t^5.282/g2^8 + (g2^6*t^5.398)/g1^2 + g1^2*g2^14*t^5.398 + t^5.699/(g1^3*g2) + (g2^3*t^5.699)/g1 + g1*g2^7*t^5.699 + g1^3*g2^11*t^5.699 + t^5.884/(g1^2*g2^22) + t^5.884/g2^18 + (g1^2*t^5.884)/g2^14 - 2*t^6. + (g2^6*t^6.116)/g1^6 + (2*g2^14*t^6.116)/g1^2 + 2*g1^2*g2^22*t^6.116 + g1^6*g2^30*t^6.116 + t^6.301/(g1*g2^7) + (g1*t^6.301)/g2^3 + (g2^7*t^6.417)/g1^3 + g1^3*g2^19*t^6.417 + t^6.602/(g1^2*g2^14) + (2*t^6.602)/g2^10 + (g1^2*t^6.602)/g2^6 + t^6.718/g1^4 + g2^8*t^6.718 + g1^4*g2^16*t^6.718 + (g2^22*t^6.834)/g1^2 + g1^2*g2^30*t^6.834 + t^7.019/(g1^5*g2^7) + t^7.019/(g1^3*g2^3) + (2*g2*t^7.019)/g1 + 2*g1*g2^5*t^7.019 + g1^3*g2^9*t^7.019 + g1^5*g2^13*t^7.019 + t^7.32/(g1^2*g2^6) + t^7.32/g2^2 + g1^2*g2^2*t^7.32 + (g2^8*t^7.436)/g1^4 + 2*g2^16*t^7.436 + g1^4*g2^24*t^7.436 + (g2*t^7.737)/g1^5 + (g2^5*t^7.737)/g1^3 + (2*g2^9*t^7.737)/g1 + 2*g1*g2^13*t^7.737 + g1^3*g2^17*t^7.737 + g1^5*g2^21*t^7.737 + t^7.923/(g1^4*g2^20) + t^7.923/(g1^2*g2^16) + (3*t^7.923)/g2^12 + (g1^2*t^7.923)/g2^8 + (g1^4*t^7.923)/g2^4 - (2*g2^2*t^8.039)/g1^2 - 2*g1^2*g2^10*t^8.039 + (g2^8*t^8.154)/g1^8 + (2*g2^16*t^8.154)/g1^4 + 3*g2^24*t^8.154 + 2*g1^4*g2^32*t^8.154 + g1^8*g2^40*t^8.154 + t^8.34/(g1^3*g2^5) + g1^3*g2^7*t^8.34 + (g2^9*t^8.455)/g1^5 + (g2^17*t^8.455)/g1 + g1*g2^21*t^8.455 + g1^5*g2^29*t^8.455 + g1^2*t^8.641 + t^8.641/(g1^4*g2^12) + t^8.641/(g1^2*g2^8) + g1^4*g2^4*t^8.641 + (g2^2*t^8.757)/g1^6 + (g2^10*t^8.757)/g1^2 + g1^2*g2^18*t^8.757 + g1^6*g2^26*t^8.757 + t^8.826/(g1^3*g2^33) + t^8.826/(g1*g2^29) + (g1*t^8.826)/g2^25 + (g1^3*t^8.826)/g2^21 + (g2^24*t^8.872)/g1^4 + 2*g2^32*t^8.872 + g1^4*g2^40*t^8.872 - t^8.942/(g1^3*g2^15) - (3*t^8.942)/(g1*g2^11) - (3*g1*t^8.942)/g2^7 - (g1^3*t^8.942)/g2^3 - t^4.32/(g2^2*y) - t^6.359/(g1^2*y) - (g1^2*g2^8*t^6.359)/y + (g2^12*t^7.077)/y - t^7.263/(g1*g2^13*y) - (g1*t^7.263)/(g2^9*y) + (g2^5*t^7.378)/(g1*y) + (g1*g2^9*t^7.378)/y + t^7.68/(g1^2*g2^2*y) + (g1^2*g2^6*t^7.68)/y + t^7.981/(g1^3*g2^9*y) + t^7.981/(g1*g2^5*y) + (g1*t^7.981)/(g2*y) + (g1^3*g2^3*t^7.981)/y + t^8.282/(g1^2*g2^12*y) + (g1^2*t^8.282)/(g2^4*y) - (g2^2*t^8.398)/(g1^4*y) + (g2^6*t^8.398)/(g1^2*y) - (g2^10*t^8.398)/y + (g1^2*g2^14*t^8.398)/y - (g1^4*g2^18*t^8.398)/y + t^8.583/(g1*g2^15*y) + (g1*t^8.583)/(g2^11*y) + t^8.699/(g1^3*g2*y) + (g2^3*t^8.699)/(g1*y) + (g1*g2^7*t^8.699)/y + (g1^3*g2^11*t^8.699)/y + t^8.884/(g2^18*y) - (t^4.32*y)/g2^2 - (t^6.359*y)/g1^2 - g1^2*g2^8*t^6.359*y + g2^12*t^7.077*y - (t^7.263*y)/(g1*g2^13) - (g1*t^7.263*y)/g2^9 + (g2^5*t^7.378*y)/g1 + g1*g2^9*t^7.378*y + (t^7.68*y)/(g1^2*g2^2) + g1^2*g2^6*t^7.68*y + (t^7.981*y)/(g1^3*g2^9) + (t^7.981*y)/(g1*g2^5) + (g1*t^7.981*y)/g2 + g1^3*g2^3*t^7.981*y + (t^8.282*y)/(g1^2*g2^12) + (g1^2*t^8.282*y)/g2^4 - (g2^2*t^8.398*y)/g1^4 + (g2^6*t^8.398*y)/g1^2 - g2^10*t^8.398*y + g1^2*g2^14*t^8.398*y - g1^4*g2^18*t^8.398*y + (t^8.583*y)/(g1*g2^15) + (g1*t^8.583*y)/g2^11 + (t^8.699*y)/(g1^3*g2) + (g2^3*t^8.699*y)/g1 + g1*g2^7*t^8.699*y + g1^3*g2^11*t^8.699*y + (t^8.884*y)/g2^18 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
46136 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6704 | 0.8232 | 0.8144 | [M:[0.9809, 0.9756, 1.1208, 0.6759], q:[0.5821, 0.437], qb:[0.4423, 0.7802], phi:[0.4396]] | t^2.028 + t^2.638 + t^2.927 + t^2.943 + t^3.362 + t^3.651 + t^3.667 + t^3.941 + t^3.957 + t^4.055 + t^4.087 + t^4.376 + t^4.392 + t^4.665 + t^4.811 + t^4.954 + t^4.97 + t^5.275 + t^5.39 + t^5.679 + t^5.695 + t^5.854 + t^5.87 + t^5.886 + t^5.968 - 2*t^6. - t^4.319/y - t^4.319*y | detail |