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 |
---|---|---|---|---|---|---|---|---|---|
46887 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{4}M_{5}$ | 0.7035 | 0.8667 | 0.8116 | [M:[1.025, 0.875, 0.925, 1.075, 0.925], q:[0.5375, 0.4375], qb:[0.5875, 0.4875], phi:[0.4875]] | [M:[[-2], [10], [6], [-6], [6]], q:[[-3], [5]], qb:[[-7], [1]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{2}q_{1}\tilde{q}_{2}$ | -1 | t^2.625 + 2*t^2.775 + t^2.925 + 3*t^3.075 + t^4.088 + t^4.238 + 2*t^4.388 + 2*t^4.537 + 2*t^4.687 + t^4.837 + t^4.987 + t^5.25 + 2*t^5.4 + 3*t^5.55 + 3*t^5.7 + 4*t^5.85 - t^6. + 2*t^6.15 - 2*t^6.3 - t^6.45 + t^6.713 + 3*t^6.863 + 4*t^7.013 + 6*t^7.163 + 5*t^7.313 + 5*t^7.463 + 3*t^7.612 + 2*t^7.762 + t^7.875 + 2*t^8.025 + t^8.062 + 4*t^8.175 + 6*t^8.325 + 5*t^8.475 + 4*t^8.625 - t^8.775 - t^4.463/y - t^7.088/y - t^7.238/y + t^7.687/y + t^7.837/y + (2*t^8.4)/y + (2*t^8.55)/y + (5*t^8.7)/y + (6*t^8.85)/y - t^4.463*y - t^7.088*y - t^7.238*y + t^7.687*y + t^7.837*y + 2*t^8.4*y + 2*t^8.55*y + 5*t^8.7*y + 6*t^8.85*y | g1^10*t^2.625 + 2*g1^6*t^2.775 + g1^2*t^2.925 + (3*t^3.075)/g1^2 + g1^11*t^4.088 + g1^7*t^4.238 + 2*g1^3*t^4.388 + (2*t^4.537)/g1 + (2*t^4.687)/g1^5 + t^4.837/g1^9 + t^4.987/g1^13 + g1^20*t^5.25 + 2*g1^16*t^5.4 + 3*g1^12*t^5.55 + 3*g1^8*t^5.7 + 4*g1^4*t^5.85 - t^6. + (2*t^6.15)/g1^4 - (2*t^6.3)/g1^8 - t^6.45/g1^12 + g1^21*t^6.713 + 3*g1^17*t^6.863 + 4*g1^13*t^7.013 + 6*g1^9*t^7.163 + 5*g1^5*t^7.313 + 5*g1*t^7.463 + (3*t^7.612)/g1^3 + (2*t^7.762)/g1^7 + g1^30*t^7.875 + 2*g1^26*t^8.025 + t^8.062/g1^15 + 4*g1^22*t^8.175 + 6*g1^18*t^8.325 + 5*g1^14*t^8.475 + 4*g1^10*t^8.625 - g1^6*t^8.775 - (g1*t^4.463)/y - (g1^11*t^7.088)/y - (g1^7*t^7.238)/y + t^7.687/(g1^5*y) + t^7.837/(g1^9*y) + (2*g1^16*t^8.4)/y + (2*g1^12*t^8.55)/y + (5*g1^8*t^8.7)/y + (6*g1^4*t^8.85)/y - g1*t^4.463*y - g1^11*t^7.088*y - g1^7*t^7.238*y + (t^7.687*y)/g1^5 + (t^7.837*y)/g1^9 + 2*g1^16*t^8.4*y + 2*g1^12*t^8.55*y + 5*g1^8*t^8.7*y + 6*g1^4*t^8.85*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 |
---|---|---|---|---|---|---|---|---|
55247 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}M_{6}$ | 0.7059 | 0.8716 | 0.8099 | [M:[1.0273, 0.8634, 0.918, 1.082, 0.918, 0.9727], q:[0.541, 0.4317], qb:[0.5956, 0.4863], phi:[0.4863]] | t^2.59 + 2*t^2.754 + 2*t^2.918 + 2*t^3.082 + t^4.049 + t^4.213 + 2*t^4.377 + 2*t^4.541 + 2*t^4.705 + t^4.869 + t^5.033 + t^5.18 + 2*t^5.344 + 4*t^5.508 + 4*t^5.672 + 4*t^5.836 - t^4.459/y - t^4.459*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 |
---|---|---|---|---|---|---|---|---|---|
46490 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ | 0.6975 | 0.8554 | 0.8154 | [M:[1.018, 0.9098, 0.9459, 1.0541], q:[0.5271, 0.4549], qb:[0.5631, 0.491], phi:[0.491]] | t^2.729 + t^2.838 + t^2.946 + 3*t^3.054 + t^3.162 + t^4.202 + t^4.311 + 2*t^4.419 + 2*t^4.527 + 2*t^4.635 + t^4.743 + t^4.852 + t^5.459 + t^5.567 + t^5.675 + 2*t^5.784 + 2*t^5.892 - t^4.473/y - t^4.473*y | detail |