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 |
---|---|---|---|---|---|---|---|---|---|
48240 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6591 | 0.8331 | 0.7912 | [M:[0.7667, 1.15, 0.85, 0.6833, 0.6833], q:[0.85, 0.3833], qb:[0.4667, 0.7667], phi:[0.3833]] | [M:[[2], [3], [-3], [7], [7]], q:[[-3], [1]], qb:[[-4], [2]], phi:[[1]]] |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 1 | 2*t^2.05 + 2*t^2.3 + t^2.55 + 2*t^3.45 + 2*t^3.7 + 3*t^4.1 + 4*t^4.35 + 5*t^4.6 + 3*t^4.85 + t^5.1 + 4*t^5.5 + 6*t^5.75 + t^6. + 4*t^6.15 + 6*t^6.4 + 9*t^6.65 + 11*t^6.9 + 5*t^7.15 - t^7.4 + 6*t^7.55 - t^7.65 + 10*t^7.8 + 4*t^8.05 + 5*t^8.199 - t^8.3 + 8*t^8.449 - 5*t^8.55 + 13*t^8.7 - 2*t^8.8 + 19*t^8.95 - t^4.15/y - (2*t^6.2)/y - (2*t^6.45)/y + t^7.1/y + (4*t^7.35)/y + (3*t^7.6)/y + (4*t^7.85)/y + (2*t^8.1)/y - (3*t^8.25)/y + (5*t^8.75)/y - t^4.15*y - 2*t^6.2*y - 2*t^6.45*y + t^7.1*y + 4*t^7.35*y + 3*t^7.6*y + 4*t^7.85*y + 2*t^8.1*y - 3*t^8.25*y + 5*t^8.75*y | 2*g1^7*t^2.05 + 2*g1^2*t^2.3 + t^2.55/g1^3 + 2*g1^3*t^3.45 + (2*t^3.7)/g1^2 + 3*g1^14*t^4.1 + 4*g1^9*t^4.35 + 5*g1^4*t^4.6 + (3*t^4.85)/g1 + t^5.1/g1^6 + 4*g1^10*t^5.5 + 6*g1^5*t^5.75 + t^6. + 4*g1^21*t^6.15 + 6*g1^16*t^6.4 + 9*g1^11*t^6.65 + 11*g1^6*t^6.9 + 5*g1*t^7.15 - t^7.4/g1^4 + 6*g1^17*t^7.55 - t^7.65/g1^9 + 10*g1^12*t^7.8 + 4*g1^7*t^8.05 + 5*g1^28*t^8.199 - g1^2*t^8.3 + 8*g1^23*t^8.449 - (5*t^8.55)/g1^3 + 13*g1^18*t^8.7 - (2*t^8.8)/g1^8 + 19*g1^13*t^8.95 - (g1*t^4.15)/y - (2*g1^8*t^6.2)/y - (2*g1^3*t^6.45)/y + (g1^14*t^7.1)/y + (4*g1^9*t^7.35)/y + (3*g1^4*t^7.6)/y + (4*t^7.85)/(g1*y) + (2*t^8.1)/(g1^6*y) - (3*g1^15*t^8.25)/y + (5*g1^5*t^8.75)/y - g1*t^4.15*y - 2*g1^8*t^6.2*y - 2*g1^3*t^6.45*y + g1^14*t^7.1*y + 4*g1^9*t^7.35*y + 3*g1^4*t^7.6*y + (4*t^7.85*y)/g1 + (2*t^8.1*y)/g1^6 - 3*g1^15*t^8.25*y + 5*g1^5*t^8.75*y |
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 |
---|---|---|---|---|---|---|---|---|
51268 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6775 | 0.8668 | 0.7816 | [M:[0.7647, 1.147, 0.853, 0.6764, 0.6764, 0.7647], q:[0.853, 0.3823], qb:[0.4706, 0.7647], phi:[0.3823]] | 2*t^2.029 + 3*t^2.294 + t^2.559 + 2*t^3.441 + t^3.706 + 3*t^4.059 + 6*t^4.323 + 8*t^4.588 + 4*t^4.853 + t^5.118 + 4*t^5.47 + 6*t^5.735 - t^4.147/y - t^4.147*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
46393 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6384 | 0.7923 | 0.8057 | [M:[0.7685, 1.1527, 0.8473, 0.6897], q:[0.8473, 0.3842], qb:[0.463, 0.7685], phi:[0.3842]] | t^2.069 + 2*t^2.305 + t^2.542 + 2*t^3.458 + 2*t^3.695 + t^3.931 + t^4.138 + 2*t^4.375 + 4*t^4.611 + 3*t^4.847 + t^5.084 + 2*t^5.527 + 4*t^5.764 + 2*t^6. - t^4.153/y - t^4.153*y | detail |