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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2934 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6447 | 0.8462 | 0.7619 | [M:[0.985, 1.0451, 0.985, 0.7462, 0.7763, 0.7763], q:[0.7462, 0.2688], qb:[0.4774, 0.4774], phi:[0.5075]] | [M:[[4], [-12], [4], [1], [-7], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | -3 | 3*t^2.239 + 2*t^2.329 + 2*t^2.955 + 2*t^3.135 + t^3.761 + 3*t^4.387 + 6*t^4.477 + 6*t^4.568 + 3*t^4.658 + 6*t^5.194 + 4*t^5.284 + 4*t^5.374 + 4*t^5.464 + 2*t^5.91 - 3*t^6. + 4*t^6.09 + 3*t^6.271 + 5*t^6.626 + 14*t^6.716 + 8*t^6.806 + 9*t^6.897 + 4*t^6.987 + 3*t^7.342 + 7*t^7.432 + 11*t^7.523 + 12*t^7.613 + 8*t^7.703 + 6*t^7.793 - 2*t^8.058 + 3*t^8.148 - 8*t^8.239 - 4*t^8.329 + 7*t^8.419 + 5*t^8.509 + 6*t^8.6 + 5*t^8.774 + 8*t^8.865 + 8*t^8.955 - t^4.523/y - t^6.761/y - (2*t^6.852)/y + t^7.387/y + (2*t^7.477)/y + (7*t^7.568)/y + (8*t^8.194)/y + (5*t^8.284)/y + (6*t^8.374)/y + (4*t^8.464)/y + t^8.91/y - t^4.523*y - t^6.761*y - 2*t^6.852*y + t^7.387*y + 2*t^7.477*y + 7*t^7.568*y + 8*t^8.194*y + 5*t^8.284*y + 6*t^8.374*y + 4*t^8.464*y + t^8.91*y | 3*g1*t^2.239 + (2*t^2.329)/g1^7 + 2*g1^4*t^2.955 + (2*t^3.135)/g1^12 + t^3.761/g1 + 3*g1^10*t^4.387 + 6*g1^2*t^4.477 + (6*t^4.568)/g1^6 + (3*t^4.658)/g1^14 + 6*g1^5*t^5.194 + (4*t^5.284)/g1^3 + (4*t^5.374)/g1^11 + (4*t^5.464)/g1^19 + 2*g1^8*t^5.91 - 3*t^6. + (4*t^6.09)/g1^8 + (3*t^6.271)/g1^24 + 5*g1^11*t^6.626 + 14*g1^3*t^6.716 + (8*t^6.806)/g1^5 + (9*t^6.897)/g1^13 + (4*t^6.987)/g1^21 + 3*g1^14*t^7.342 + 7*g1^6*t^7.432 + (11*t^7.523)/g1^2 + (12*t^7.613)/g1^10 + (8*t^7.703)/g1^18 + (6*t^7.793)/g1^26 - 2*g1^17*t^8.058 + 3*g1^9*t^8.148 - 8*g1*t^8.239 - (4*t^8.329)/g1^7 + (7*t^8.419)/g1^15 + (5*t^8.509)/g1^23 + (6*t^8.6)/g1^31 + 5*g1^20*t^8.774 + 8*g1^12*t^8.865 + 8*g1^4*t^8.955 - t^4.523/(g1^2*y) - t^6.761/(g1*y) - (2*t^6.852)/(g1^9*y) + (g1^10*t^7.387)/y + (2*g1^2*t^7.477)/y + (7*t^7.568)/(g1^6*y) + (8*g1^5*t^8.194)/y + (5*t^8.284)/(g1^3*y) + (6*t^8.374)/(g1^11*y) + (4*t^8.464)/(g1^19*y) + (g1^8*t^8.91)/y - (t^4.523*y)/g1^2 - (t^6.761*y)/g1 - (2*t^6.852*y)/g1^9 + g1^10*t^7.387*y + 2*g1^2*t^7.477*y + (7*t^7.568*y)/g1^6 + 8*g1^5*t^8.194*y + (5*t^8.284*y)/g1^3 + (6*t^8.374*y)/g1^11 + (4*t^8.464*y)/g1^19 + g1^8*t^8.91*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 |
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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 |
---|---|---|---|---|---|---|---|---|---|
1904 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6272 | 0.8147 | 0.7699 | [M:[0.978, 1.0661, 0.978, 0.7445, 0.7886], q:[0.7445, 0.2775], qb:[0.4669, 0.4669], phi:[0.511]] | 3*t^2.233 + t^2.366 + 2*t^2.934 + 2*t^3.198 + t^3.634 + t^3.767 + 3*t^4.335 + 6*t^4.467 + 3*t^4.599 + t^4.731 + 6*t^5.167 + 2*t^5.3 + 4*t^5.432 + 2*t^5.564 + 5*t^5.868 - 2*t^6. - t^4.533/y - t^4.533*y | detail |