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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6089 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{8}$ + ${ }M_{7}^{2}$ + ${ }M_{6}X_{1}$ + ${ }M_{9}\phi_{1}^{2}$ | 0.6096 | 0.7549 | 0.8074 | [X:[1.442], M:[0.7461, 1.022, 0.978, 0.79, 1.21, 0.558, 1.0, 1.022, 1.116], q:[0.743, 0.511], qb:[0.279, 0.699], phi:[0.442]] | [X:[[2]], M:[[26], [-18], [18], [-10], [10], [-2], [0], [-18], [-4]], q:[[-17], [-9]], qb:[[-1], [19]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{8}$, ${ }M_{9}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{8}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{9}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{9}$, ${ }\phi_{1}q_{1}^{2}$ | ${}$ | -2 | t^2.238 + t^2.37 + t^3. + 2*t^3.066 + t^3.348 + t^3.63 + t^3.696 + t^4.26 + t^4.326 + 2*t^4.392 + t^4.476 + t^4.956 + t^5.088 + t^5.238 + t^5.37 + t^5.436 + t^5.52 + t^5.586 + t^5.652 + t^5.718 + t^5.784 - 2*t^6. + 2*t^6.066 + 2*t^6.132 + 2*t^6.414 + t^6.498 + t^6.63 + 2*t^6.696 + t^6.715 + 2*t^6.762 + t^7.26 + t^7.326 + 3*t^7.392 + 3*t^7.458 + t^7.476 + t^7.542 - t^7.674 + t^7.758 + t^7.824 + t^7.89 + 2*t^7.956 + 2*t^8.022 + 2*t^8.088 + 2*t^8.154 - 2*t^8.238 - t^8.304 - 3*t^8.37 + t^8.436 + t^8.502 + t^8.52 + 2*t^8.586 + 3*t^8.652 + 2*t^8.718 + t^8.737 + 4*t^8.784 + 2*t^8.85 - 2*t^8.934 + t^8.953 - t^4.326/y - t^6.564/y + t^7.26/y - t^7.392/y + t^7.608/y + t^8.088/y + t^8.238/y + (2*t^8.304)/y + t^8.37/y + (2*t^8.436)/y + t^8.586/y + t^8.718/y - t^8.802/y + t^8.868/y + t^8.934/y - t^4.326*y - t^6.564*y + t^7.26*y - t^7.392*y + t^7.608*y + t^8.088*y + t^8.238*y + 2*t^8.304*y + t^8.37*y + 2*t^8.436*y + t^8.586*y + t^8.718*y - t^8.802*y + t^8.868*y + t^8.934*y | g1^26*t^2.238 + t^2.37/g1^10 + t^3. + (2*t^3.066)/g1^18 + t^3.348/g1^4 + g1^10*t^3.63 + t^3.696/g1^8 + g1^20*t^4.26 + g1^2*t^4.326 + (2*t^4.392)/g1^16 + g1^52*t^4.476 + g1^12*t^4.956 + t^5.088/g1^24 + g1^26*t^5.238 + t^5.37/g1^10 + t^5.436/g1^28 + g1^40*t^5.52 + g1^22*t^5.586 + g1^4*t^5.652 + t^5.718/g1^14 + t^5.784/g1^32 - 2*t^6. + (2*t^6.066)/g1^18 + (2*t^6.132)/g1^36 + (2*t^6.414)/g1^22 + g1^46*t^6.498 + g1^10*t^6.63 + (2*t^6.696)/g1^8 + g1^78*t^6.715 + (2*t^6.762)/g1^26 + g1^20*t^7.26 + g1^2*t^7.326 + (3*t^7.392)/g1^16 + (3*t^7.458)/g1^34 + g1^52*t^7.476 + g1^34*t^7.542 - t^7.674/g1^2 + g1^66*t^7.758 + g1^48*t^7.824 + g1^30*t^7.89 + 2*g1^12*t^7.956 + (2*t^8.022)/g1^6 + (2*t^8.088)/g1^24 + (2*t^8.154)/g1^42 - 2*g1^26*t^8.238 - g1^8*t^8.304 - (3*t^8.37)/g1^10 + t^8.436/g1^28 + t^8.502/g1^46 + g1^40*t^8.52 + 2*g1^22*t^8.586 + 3*g1^4*t^8.652 + (2*t^8.718)/g1^14 + g1^72*t^8.737 + (4*t^8.784)/g1^32 + (2*t^8.85)/g1^50 - 2*g1^18*t^8.934 + g1^104*t^8.953 - (g1^2*t^4.326)/y - (g1^28*t^6.564)/y + (g1^20*t^7.26)/y - t^7.392/(g1^16*y) + (g1^16*t^7.608)/y + t^8.088/(g1^24*y) + (g1^26*t^8.238)/y + (2*g1^8*t^8.304)/y + t^8.37/(g1^10*y) + (2*t^8.436)/(g1^28*y) + (g1^22*t^8.586)/y + t^8.718/(g1^14*y) - (g1^54*t^8.802)/y + (g1^36*t^8.868)/y + (g1^18*t^8.934)/y - g1^2*t^4.326*y - g1^28*t^6.564*y + g1^20*t^7.26*y - (t^7.392*y)/g1^16 + g1^16*t^7.608*y + (t^8.088*y)/g1^24 + g1^26*t^8.238*y + 2*g1^8*t^8.304*y + (t^8.37*y)/g1^10 + (2*t^8.436*y)/g1^28 + g1^22*t^8.586*y + (t^8.718*y)/g1^14 - g1^54*t^8.802*y + g1^36*t^8.868*y + g1^18*t^8.934*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 |
---|---|---|---|---|---|---|---|---|---|
4558 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{8}$ + ${ }M_{7}^{2}$ + ${ }M_{6}X_{1}$ | 0.62 | 0.7726 | 0.8025 | [X:[1.4414], M:[0.7379, 1.0276, 0.9724, 0.7931, 1.2069, 0.5586, 1.0, 1.0276], q:[0.7483, 0.5138], qb:[0.2793, 0.6931], phi:[0.4414]] | t^2.214 + t^2.379 + t^2.648 + t^3. + 2*t^3.083 + t^3.621 + t^3.704 + t^4.241 + t^4.324 + 2*t^4.407 + t^4.427 + t^4.862 + t^4.945 + t^5.028 + t^5.111 + t^5.214 + t^5.296 + t^5.379 + t^5.462 + t^5.482 + 2*t^5.648 + 2*t^5.731 + t^5.814 - 2*t^6. - t^4.324/y - t^4.324*y | detail |