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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59001 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.3494 | 1.5258 | 0.8844 | [X:[1.4134], M:[0.8799, 0.8177], q:[0.6459, 0.4148], qb:[0.7675, 0.412], phi:[0.2933]] | [X:[[0, 4]], M:[[0, -6], [3, -15]], q:[[1, -3], [-2, 8]], qb:[[-1, 7], [2, 0]], phi:[[0, -2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.45 + t^2.48 + 2*t^2.64 + t^3.17 + t^4.05 + 3*t^4.24 + t^4.43 + t^4.91 + t^4.93 + t^4.96 + 2*t^5.09 + 3*t^5.12 + 3*t^5.28 + t^5.31 + t^5.63 + 2*t^5.65 + t^5.81 - 2*t^6. + 2*t^6.35 + t^6.37 + t^6.51 + 2*t^6.53 + 3*t^6.69 + 4*t^6.72 + 4*t^6.88 + t^6.91 + t^7.23 + t^7.36 + t^7.39 + 4*t^7.41 + t^7.44 + 2*t^7.55 + 2*t^7.57 + 3*t^7.6 + 3*t^7.73 + 4*t^7.76 + t^7.79 + 4*t^7.92 - t^7.95 + t^8.08 + 2*t^8.11 + t^8.13 + t^8.27 + 4*t^8.29 - t^8.45 + 3*t^8.48 - 3*t^8.64 + 2*t^8.67 + 2*t^8.8 + t^8.83 + 2*t^8.85 + t^8.96 + 4*t^8.99 + t^8.64/y^2 - t^3.88/y - t^4.76/y - t^6.33/y - t^6.36/y - (2*t^6.52)/y - t^7.05/y - t^7.21/y - (2*t^7.4)/y + (2*t^8.09)/y + t^8.12/y + t^8.28/y + t^8.63/y + t^8.65/y - t^8.79/y + t^8.81/y - t^8.84/y - (2*t^8.97)/y - t^3.88*y - t^4.76*y - t^6.33*y - t^6.36*y - 2*t^6.52*y - t^7.05*y - t^7.21*y - 2*t^7.4*y + 2*t^8.09*y + t^8.12*y + t^8.28*y + t^8.63*y + t^8.65*y - t^8.79*y + t^8.81*y - t^8.84*y - 2*t^8.97*y + t^8.64*y^2 | (g1^3*t^2.45)/g2^15 + g2^8*t^2.48 + (2*t^2.64)/g2^6 + (g1^3*t^3.17)/g2^3 + (g1^3*t^4.05)/g2^5 + 3*g2^4*t^4.24 + (g2^13*t^4.43)/g1^3 + (g1^6*t^4.91)/g2^30 + (g1^3*t^4.93)/g2^7 + g2^16*t^4.96 + (2*g1^3*t^5.09)/g2^21 + 3*g2^2*t^5.12 + (3*t^5.28)/g2^12 + (g2^11*t^5.31)/g1^3 + (g1^6*t^5.63)/g2^18 + 2*g1^3*g2^5*t^5.65 + (g1^3*t^5.81)/g2^9 - 2*t^6. + (2*g1^6*t^6.35)/g2^6 + (g2^18*t^6.37)/g1^6 + (g1^6*t^6.51)/g2^20 + 2*g1^3*g2^3*t^6.53 + (3*g1^3*t^6.69)/g2^11 + 4*g2^12*t^6.72 + (4*t^6.88)/g2^2 + (g2^21*t^6.91)/g1^3 + (g1^6*t^7.23)/g2^8 + (g1^9*t^7.36)/g2^45 + (g1^6*t^7.39)/g2^22 + 4*g1^3*g2*t^7.41 + g2^24*t^7.44 + (2*g1^6*t^7.55)/g2^36 + (2*g1^3*t^7.57)/g2^13 + 3*g2^10*t^7.6 + (3*g1^3*t^7.73)/g2^27 + (4*t^7.76)/g2^4 + (g2^19*t^7.79)/g1^3 + (4*t^7.92)/g2^18 - (g2^5*t^7.95)/g1^3 + (g1^9*t^8.08)/g2^33 + (2*g1^6*t^8.11)/g2^10 + 2*g1^3*g2^13*t^8.13 - (g2^14*t^8.13)/g1^6 + (g1^6*t^8.27)/g2^24 + (4*g1^3*t^8.29)/g2 - (g1^3*t^8.45)/g2^15 + 3*g2^8*t^8.48 - (3*t^8.64)/g2^6 + (2*g2^17*t^8.67)/g1^3 + (2*g1^9*t^8.8)/g2^21 + 3*g1^6*g2^2*t^8.83 - (2*g2^3*t^8.83)/g1^3 + (2*g2^26*t^8.85)/g1^6 + (g1^9*t^8.96)/g2^35 + (4*g1^6*t^8.99)/g2^12 + t^8.64/(g2^6*y^2) - t^3.88/(g2^2*y) - t^4.76/(g2^4*y) - (g1^3*t^6.33)/(g2^17*y) - (g2^6*t^6.36)/y - (2*t^6.52)/(g2^8*y) - (g1^3*t^7.05)/(g2^5*y) - (g1^3*t^7.21)/(g2^19*y) - (2*t^7.4)/(g2^10*y) + (2*g1^3*t^8.09)/(g2^21*y) + (g2^2*t^8.12)/y + t^8.28/(g2^12*y) + (g1^6*t^8.63)/(g2^18*y) + (g1^3*g2^5*t^8.65)/y - (g1^6*t^8.79)/(g2^32*y) + (g1^3*t^8.81)/(g2^9*y) - (g2^14*t^8.84)/y - (2*g1^3*t^8.97)/(g2^23*y) - (t^3.88*y)/g2^2 - (t^4.76*y)/g2^4 - (g1^3*t^6.33*y)/g2^17 - g2^6*t^6.36*y - (2*t^6.52*y)/g2^8 - (g1^3*t^7.05*y)/g2^5 - (g1^3*t^7.21*y)/g2^19 - (2*t^7.4*y)/g2^10 + (2*g1^3*t^8.09*y)/g2^21 + g2^2*t^8.12*y + (t^8.28*y)/g2^12 + (g1^6*t^8.63*y)/g2^18 + g1^3*g2^5*t^8.65*y - (g1^6*t^8.79*y)/g2^32 + (g1^3*t^8.81*y)/g2^9 - g2^14*t^8.84*y - (2*g1^3*t^8.97*y)/g2^23 + (t^8.64*y^2)/g2^6 |
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 |
---|---|---|---|---|---|---|---|---|---|
57632 | SU3adj1nf2 | ${}\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.3357 | 1.5044 | 0.8879 | [X:[1.4001], M:[0.8998], q:[0.6555, 0.389], qb:[0.7446, 0.4113], phi:[0.2999]] | t^2.4 + 2*t^2.7 + t^3.2 + t^3.4 + t^4.1 + 3*t^4.2 + t^4.3 + t^4.8 + 3*t^5.1 + t^5.2 + 3*t^5.4 + 2*t^5.6 + t^5.8 + t^5.9 - 2*t^6. - t^3.9/y - t^4.8/y - t^3.9*y - t^4.8*y | detail |