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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56488 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ | 0.6964 | 0.8727 | 0.798 | [M:[1.0073, 1.0896, 1.0896, 0.9104, 0.7313, 0.7166, 0.9104], q:[0.4963, 0.4963], qb:[0.4141, 0.7724], phi:[0.4552]] | [M:[[-22], [4], [4], [-4], [-12], [32], [-4]], q:[[11], [11]], qb:[[-15], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{1}M_{5}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$ | ${}M_{5}q_{1}\tilde{q}_{2}$ | -4 | t^2.15 + t^2.194 + 3*t^2.731 + t^3.022 + t^3.559 + t^3.806 + 2*t^4.097 + t^4.3 + 4*t^4.344 + t^4.388 + 3*t^4.881 + 3*t^4.925 + t^5.172 + t^5.216 + 6*t^5.463 + t^5.709 + 2*t^5.753 + t^5.956 - 4*t^6. + t^6.044 + 4*t^6.291 + t^6.449 + 4*t^6.493 + 4*t^6.537 + 2*t^6.581 + 4*t^6.828 + 3*t^7.031 + 9*t^7.075 + 3*t^7.119 + t^7.322 - t^7.366 + t^7.41 + 2*t^7.612 + 6*t^7.656 + t^7.859 + 3*t^7.903 + 2*t^7.947 + t^8.106 - 3*t^8.15 + 6*t^8.194 + t^8.238 + 4*t^8.441 + 4*t^8.485 + t^8.599 + 4*t^8.643 + 9*t^8.687 - 10*t^8.731 + 3*t^8.775 - 2*t^8.978 - t^4.366/y - t^6.515/y - t^6.559/y - t^7.097/y + (2*t^7.344)/y - t^7.388/y + t^7.634/y + (3*t^7.881)/y + (3*t^7.925)/y + (2*t^8.172)/y + (2*t^8.216)/y + (3*t^8.463)/y - t^8.665/y + (3*t^8.753)/y + t^8.956/y - t^4.366*y - t^6.515*y - t^6.559*y - t^7.097*y + 2*t^7.344*y - t^7.388*y + t^7.634*y + 3*t^7.881*y + 3*t^7.925*y + 2*t^8.172*y + 2*t^8.216*y + 3*t^8.463*y - t^8.665*y + 3*t^8.753*y + t^8.956*y | g1^32*t^2.15 + t^2.194/g1^12 + (3*t^2.731)/g1^4 + t^3.022/g1^22 + t^3.559/g1^14 + g1^12*t^3.806 + (2*t^4.097)/g1^6 + g1^64*t^4.3 + 4*g1^20*t^4.344 + t^4.388/g1^24 + 3*g1^28*t^4.881 + (3*t^4.925)/g1^16 + g1^10*t^5.172 + t^5.216/g1^34 + (6*t^5.463)/g1^8 + g1^18*t^5.709 + (2*t^5.753)/g1^26 + g1^44*t^5.956 - 4*t^6. + t^6.044/g1^44 + (4*t^6.291)/g1^18 + g1^96*t^6.449 + 4*g1^52*t^6.493 + 4*g1^8*t^6.537 + (2*t^6.581)/g1^36 + (4*t^6.828)/g1^10 + 3*g1^60*t^7.031 + 9*g1^16*t^7.075 + (3*t^7.119)/g1^28 + g1^42*t^7.322 - t^7.366/g1^2 + t^7.41/g1^46 + 2*g1^24*t^7.612 + (6*t^7.656)/g1^20 + g1^50*t^7.859 + 3*g1^6*t^7.903 + (2*t^7.947)/g1^38 + g1^76*t^8.106 - 3*g1^32*t^8.15 + (6*t^8.194)/g1^12 + t^8.238/g1^56 + 4*g1^14*t^8.441 + (4*t^8.485)/g1^30 + g1^128*t^8.599 + 4*g1^84*t^8.643 + 9*g1^40*t^8.687 - (10*t^8.731)/g1^4 + (3*t^8.775)/g1^48 - 2*g1^22*t^8.978 - t^4.366/(g1^2*y) - (g1^30*t^6.515)/y - t^6.559/(g1^14*y) - t^7.097/(g1^6*y) + (2*g1^20*t^7.344)/y - t^7.388/(g1^24*y) + (g1^2*t^7.634)/y + (3*g1^28*t^7.881)/y + (3*t^7.925)/(g1^16*y) + (2*g1^10*t^8.172)/y + (2*t^8.216)/(g1^34*y) + (3*t^8.463)/(g1^8*y) - (g1^62*t^8.665)/y + (3*t^8.753)/(g1^26*y) + (g1^44*t^8.956)/y - (t^4.366*y)/g1^2 - g1^30*t^6.515*y - (t^6.559*y)/g1^14 - (t^7.097*y)/g1^6 + 2*g1^20*t^7.344*y - (t^7.388*y)/g1^24 + g1^2*t^7.634*y + 3*g1^28*t^7.881*y + (3*t^7.925*y)/g1^16 + 2*g1^10*t^8.172*y + (2*t^8.216*y)/g1^34 + (3*t^8.463*y)/g1^8 - g1^62*t^8.665*y + (3*t^8.753*y)/g1^26 + g1^44*t^8.956*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 |
---|---|---|---|---|---|---|---|---|---|
53324 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6883 | 0.8591 | 0.8011 | [M:[1.0127, 1.0886, 1.0886, 0.9114, 0.7342, 0.7087], q:[0.4936, 0.4936], qb:[0.4178, 0.7721], phi:[0.4557]] | t^2.126 + t^2.203 + 2*t^2.734 + t^3.038 + t^3.266 + t^3.57 + t^3.797 + 2*t^4.101 + t^4.252 + 4*t^4.329 + t^4.405 + 2*t^4.86 + 2*t^4.937 + t^5.164 + t^5.241 + t^5.392 + 4*t^5.468 + t^5.696 + t^5.772 + t^5.924 - 2*t^6. - t^4.367/y - t^4.367*y | detail |