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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61052 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.1497 | 1.3051 | 0.8809 | [X:[1.5123], M:[0.6822, 0.7808, 0.9754], q:[0.837, 0.3986], qb:[0.3822, 0.9191], phi:[0.2438]] | [X:[[0, 2]], M:[[0, -11], [0, 5], [0, -4]], q:[[-1, 1], [-1, 11]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }M_{3}^{2}$ | ${}\phi_{1}^{5}q_{2}\tilde{q}_{1}$ | -2 | t^2.05 + t^2.19 + 2*t^2.34 + t^2.93 + t^3.81 + t^4.09 + t^4.24 + 3*t^4.39 + 3*t^4.54 + 3*t^4.68 + t^4.97 + t^5.12 + 3*t^5.27 + 2*t^5.63 + 2*t^5.78 + t^5.85 - 2*t^6. + t^6.14 + t^6.15 + t^6.29 + 3*t^6.44 + 4*t^6.58 + 6*t^6.73 + 5*t^6.88 + t^7.02 + 4*t^7.03 + t^7.17 + 3*t^7.32 + 3*t^7.46 + 4*t^7.61 + 2*t^7.68 + 2*t^7.83 + t^7.9 + 4*t^7.98 - 2*t^8.05 + 4*t^8.12 + 3*t^8.19 + t^8.33 - 5*t^8.34 + 3*t^8.48 + t^8.49 + 4*t^8.63 + 5*t^8.78 + 3*t^8.93 + t^8.19/y^2 - t^8.78/y^2 - t^8.93/y^2 - t^3.73/y - t^4.46/y - t^5.78/y - t^5.93/y - (2*t^6.07)/y - t^6.51/y - (2*t^6.66)/y - t^6.81/y + t^7.24/y + t^7.39/y + (2*t^7.54)/y + t^7.68/y - t^7.83/y - t^8.12/y - (2*t^8.42)/y - t^8.56/y - (2*t^8.7)/y - (2*t^8.85)/y - t^3.73*y - t^4.46*y - t^5.78*y - t^5.93*y - 2*t^6.07*y - t^6.51*y - 2*t^6.66*y - t^6.81*y + t^7.24*y + t^7.39*y + 2*t^7.54*y + t^7.68*y - t^7.83*y - t^8.12*y - 2*t^8.42*y - t^8.56*y - 2*t^8.7*y - 2*t^8.85*y + t^8.19*y^2 - t^8.78*y^2 - t^8.93*y^2 | t^2.05/g2^11 + t^2.19/g2^3 + 2*g2^5*t^2.34 + t^2.93/g2^4 + g2^3*t^3.81 + t^4.09/g2^22 + t^4.24/g2^14 + (3*t^4.39)/g2^6 + 3*g2^2*t^4.54 + 3*g2^10*t^4.68 + t^4.97/g2^15 + t^5.12/g2^7 + 3*g2*t^5.27 + (g1^3*t^5.63)/g2^21 + (g2^22*t^5.63)/g1^3 + (g1^3*t^5.78)/g2^13 + (g2^30*t^5.78)/g1^3 + t^5.85/g2^8 - 2*t^6. + t^6.14/g2^33 + g2^8*t^6.15 + t^6.29/g2^25 + (3*t^6.44)/g2^17 + (4*t^6.58)/g2^9 + (6*t^6.73)/g2 + 5*g2^7*t^6.88 + t^7.02/g2^26 + 4*g2^15*t^7.03 + t^7.17/g2^18 + (3*t^7.32)/g2^10 + (3*t^7.46)/g2^2 + 4*g2^6*t^7.61 + (g1^3*t^7.68)/g2^32 + (g2^11*t^7.68)/g1^3 + (g1^3*t^7.83)/g2^24 + (g2^19*t^7.83)/g1^3 + t^7.9/g2^19 + (2*g1^3*t^7.98)/g2^16 + (2*g2^27*t^7.98)/g1^3 - (2*t^8.05)/g2^11 + (2*g1^3*t^8.12)/g2^8 + (2*g2^35*t^8.12)/g1^3 + t^8.19/g2^44 + (2*t^8.19)/g2^3 + t^8.33/g2^36 - 5*g2^5*t^8.34 + (3*t^8.48)/g2^28 + g2^13*t^8.49 + (4*t^8.63)/g2^20 + (5*t^8.78)/g2^12 + (3*t^8.93)/g2^4 + t^8.19/(g2^3*y^2) - t^8.78/(g2^12*y^2) - t^8.93/(g2^4*y^2) - t^3.73/(g2*y) - t^4.46/(g2^2*y) - t^5.78/(g2^12*y) - t^5.93/(g2^4*y) - (2*g2^4*t^6.07)/y - t^6.51/(g2^13*y) - (2*t^6.66)/(g2^5*y) - (g2^3*t^6.81)/y + t^7.24/(g2^14*y) + t^7.39/(g2^6*y) + (2*g2^2*t^7.54)/y + (g2^10*t^7.68)/y - t^7.83/(g2^23*y) - t^8.12/(g2^7*y) - (2*g2^9*t^8.42)/y - t^8.56/(g2^24*y) - (2*t^8.7)/(g2^16*y) - (2*t^8.85)/(g2^8*y) - (t^3.73*y)/g2 - (t^4.46*y)/g2^2 - (t^5.78*y)/g2^12 - (t^5.93*y)/g2^4 - 2*g2^4*t^6.07*y - (t^6.51*y)/g2^13 - (2*t^6.66*y)/g2^5 - g2^3*t^6.81*y + (t^7.24*y)/g2^14 + (t^7.39*y)/g2^6 + 2*g2^2*t^7.54*y + g2^10*t^7.68*y - (t^7.83*y)/g2^23 - (t^8.12*y)/g2^7 - 2*g2^9*t^8.42*y - (t^8.56*y)/g2^24 - (2*t^8.7*y)/g2^16 - (2*t^8.85*y)/g2^8 + (t^8.19*y^2)/g2^3 - (t^8.78*y^2)/g2^12 - (t^8.93*y^2)/g2^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
57926 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | 1.1477 | 1.3025 | 0.8812 | [X:[1.5082], M:[0.7049, 0.7705], q:[0.8497, 0.3907], qb:[0.3798, 0.9044], phi:[0.2459]] | t^2.11 + t^2.21 + 2*t^2.31 + t^3.05 + t^3.79 + t^4.23 + t^4.33 + 3*t^4.43 + 3*t^4.52 + 3*t^4.62 + t^5.16 + 2*t^5.26 + 2*t^5.36 + 2*t^5.63 + 2*t^5.73 - 2*t^6. - t^3.74/y - t^4.48/y - t^5.85/y - t^5.95/y - t^3.74*y - t^4.48*y - t^5.85*y - t^5.95*y | detail |