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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3016 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{7}$ | 0.6501 | 0.8149 | 0.7978 | [M:[1.1817, 1.2122, 0.7572, 0.8183, 0.8183, 0.7267, 0.8183], q:[0.8031, 0.4397], qb:[0.3786, 0.8031], phi:[0.3939]] | [M:[[-6], [4], [-14], [6], [6], [-24], [6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{6}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{6}q_{1}q_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ | ${}\phi_{1}\tilde{q}_{2}^{2}$ | -2 | t^2.18 + t^2.272 + 3*t^2.455 + t^3.453 + 2*t^3.637 + t^3.728 + t^4.36 + t^4.452 + t^4.543 + 3*t^4.635 + 3*t^4.727 + t^4.818 + 6*t^4.91 + t^5.634 + t^5.725 + t^5.817 + 4*t^5.908 - 2*t^6. + 4*t^6.092 + 2*t^6.183 + t^6.54 + t^6.632 + t^6.724 + 4*t^6.815 + 4*t^6.907 + 3*t^6.998 + 6*t^7.09 + 3*t^7.182 + t^7.273 + 9*t^7.365 + t^7.814 + t^7.905 + 2*t^7.997 + 3*t^8.089 + t^8.18 - t^8.272 + 5*t^8.363 - 7*t^8.455 + 5*t^8.547 + 2*t^8.638 + t^8.721 + t^8.812 + t^8.904 + 4*t^8.995 - t^4.182/y - t^6.362/y - t^6.453/y - (2*t^6.637)/y + t^7.452/y + (3*t^7.635)/y + (5*t^7.727)/y + (4*t^7.91)/y + t^8.002/y - t^8.542/y + (4*t^8.908)/y - t^4.182*y - t^6.362*y - t^6.453*y - 2*t^6.637*y + t^7.452*y + 3*t^7.635*y + 5*t^7.727*y + 4*t^7.91*y + t^8.002*y - t^8.542*y + 4*t^8.908*y | t^2.18/g1^24 + t^2.272/g1^14 + 3*g1^6*t^2.455 + t^3.453/g1^16 + 2*g1^4*t^3.637 + g1^14*t^3.728 + t^4.36/g1^48 + t^4.452/g1^38 + t^4.543/g1^28 + (3*t^4.635)/g1^18 + (3*t^4.727)/g1^8 + g1^2*t^4.818 + 6*g1^12*t^4.91 + t^5.634/g1^40 + t^5.725/g1^30 + t^5.817/g1^20 + (4*t^5.908)/g1^10 - 2*t^6. + 4*g1^10*t^6.092 + 2*g1^20*t^6.183 + t^6.54/g1^72 + t^6.632/g1^62 + t^6.724/g1^52 + (4*t^6.815)/g1^42 + (4*t^6.907)/g1^32 + (3*t^6.998)/g1^22 + (6*t^7.09)/g1^12 + (3*t^7.182)/g1^2 + g1^8*t^7.273 + 9*g1^18*t^7.365 + t^7.814/g1^64 + t^7.905/g1^54 + (2*t^7.997)/g1^44 + (3*t^8.089)/g1^34 + t^8.18/g1^24 - t^8.272/g1^14 + (5*t^8.363)/g1^4 - 7*g1^6*t^8.455 + 5*g1^16*t^8.547 + 2*g1^26*t^8.638 + t^8.721/g1^96 + t^8.812/g1^86 + t^8.904/g1^76 + (4*t^8.995)/g1^66 - t^4.182/(g1^2*y) - t^6.362/(g1^26*y) - t^6.453/(g1^16*y) - (2*g1^4*t^6.637)/y + t^7.452/(g1^38*y) + (3*t^7.635)/(g1^18*y) + (5*t^7.727)/(g1^8*y) + (4*g1^12*t^7.91)/y + (g1^22*t^8.002)/y - t^8.542/(g1^50*y) + (4*t^8.908)/(g1^10*y) - (t^4.182*y)/g1^2 - (t^6.362*y)/g1^26 - (t^6.453*y)/g1^16 - 2*g1^4*t^6.637*y + (t^7.452*y)/g1^38 + (3*t^7.635*y)/g1^18 + (5*t^7.727*y)/g1^8 + 4*g1^12*t^7.91*y + g1^22*t^8.002*y - (t^8.542*y)/g1^50 + (4*t^8.908*y)/g1^10 |
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 |
---|---|---|---|---|---|---|---|---|---|
1961 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6349 | 0.7889 | 0.8048 | [M:[1.1787, 1.2142, 0.7503, 0.8213, 0.8213, 0.7147], q:[0.8036, 0.4462], qb:[0.3751, 0.8036], phi:[0.3929]] | t^2.144 + t^2.251 + 2*t^2.464 + t^3.429 + t^3.536 + 2*t^3.643 + t^3.749 + t^4.288 + t^4.395 + t^4.502 + 2*t^4.608 + 2*t^4.715 + t^4.821 + 3*t^4.928 + t^5.574 + 2*t^5.68 + 2*t^5.787 + 3*t^5.893 - t^4.179/y - t^4.179*y | detail |