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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60071 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.4323 | 1.6571 | 0.8643 | [X:[], M:[0.8661], q:[0.3726, 0.6405], qb:[0.4934, 0.4148], phi:[0.3464]] | [X:[], M:[[-5]], q:[[-6], [4]], qb:[[1], [13]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{5}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.08 + t^2.36 + 2*t^2.6 + t^3.12 + t^3.17 + t^3.4 + t^3.64 + t^4.16 + t^4.21 + 3*t^4.44 + 3*t^4.68 + t^4.72 + 2*t^4.96 + t^5.01 + 4*t^5.2 + 3*t^5.24 + 3*t^5.48 + t^5.53 + 3*t^5.72 + 2*t^5.76 + t^6.05 + 3*t^6.24 + 3*t^6.28 + t^6.33 + t^6.47 + 4*t^6.52 + 2*t^6.57 + 4*t^6.76 + 4*t^6.8 + t^6.85 + 6*t^7.04 + 3*t^7.09 + 6*t^7.28 + 6*t^7.32 + 2*t^7.37 + 7*t^7.56 + 6*t^7.61 + 6*t^7.79 + 7*t^7.84 + t^7.89 - t^8.03 + 5*t^8.08 + 3*t^8.13 + t^8.17 + 6*t^8.31 + 4*t^8.36 + 5*t^8.41 + t^8.55 + 2*t^8.6 + 8*t^8.65 + t^8.69 + 6*t^8.83 + 11*t^8.88 + 3*t^8.93 - t^4.04/y - t^5.08/y - t^6.12/y - t^6.4/y - (2*t^6.64)/y - (2*t^7.16)/y - t^7.21/y + (3*t^7.96)/y + t^8.53/y + (2*t^8.76)/y - t^4.04*y - t^5.08*y - t^6.12*y - t^6.4*y - 2*t^6.64*y - 2*t^7.16*y - t^7.21*y + 3*t^7.96*y + t^8.53*y + 2*t^8.76*y | t^2.08/g1^4 + g1^7*t^2.36 + (2*t^2.6)/g1^5 + t^3.12/g1^6 + g1^17*t^3.17 + g1^5*t^3.4 + t^3.64/g1^7 + t^4.16/g1^8 + g1^15*t^4.21 + 3*g1^3*t^4.44 + (3*t^4.68)/g1^9 + g1^14*t^4.72 + 2*g1^2*t^4.96 + g1^25*t^5.01 + (4*t^5.2)/g1^10 + 3*g1^13*t^5.24 + 3*g1*t^5.48 + g1^24*t^5.53 + (3*t^5.72)/g1^11 + 2*g1^12*t^5.76 + g1^23*t^6.05 + (3*t^6.24)/g1^12 + 3*g1^11*t^6.28 + g1^34*t^6.33 + t^6.47/g1^24 + (4*t^6.52)/g1 + 2*g1^22*t^6.57 + (4*t^6.76)/g1^13 + 4*g1^10*t^6.8 + g1^33*t^6.85 + (6*t^7.04)/g1^2 + 3*g1^21*t^7.09 + (6*t^7.28)/g1^14 + 6*g1^9*t^7.32 + 2*g1^32*t^7.37 + (7*t^7.56)/g1^3 + 6*g1^20*t^7.61 + (6*t^7.79)/g1^15 + 7*g1^8*t^7.84 + g1^31*t^7.89 - t^8.03/g1^27 + (5*t^8.08)/g1^4 + 3*g1^19*t^8.13 + g1^42*t^8.17 + (6*t^8.31)/g1^16 + 4*g1^7*t^8.36 + 5*g1^30*t^8.41 + t^8.55/g1^28 + (2*t^8.6)/g1^5 + 8*g1^18*t^8.65 + g1^41*t^8.69 + (6*t^8.83)/g1^17 + 11*g1^6*t^8.88 + 3*g1^29*t^8.93 - t^4.04/(g1^2*y) - t^5.08/(g1^4*y) - t^6.12/(g1^6*y) - (g1^5*t^6.4)/y - (2*t^6.64)/(g1^7*y) - (2*t^7.16)/(g1^8*y) - (g1^15*t^7.21)/y + (3*g1^2*t^7.96)/y + (g1^24*t^8.53)/y + (2*g1^12*t^8.76)/y - (t^4.04*y)/g1^2 - (t^5.08*y)/g1^4 - (t^6.12*y)/g1^6 - g1^5*t^6.4*y - (2*t^6.64*y)/g1^7 - (2*t^7.16*y)/g1^8 - g1^15*t^7.21*y + 3*g1^2*t^7.96*y + g1^24*t^8.53*y + 2*g1^12*t^8.76*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 |
---|---|---|---|---|---|---|---|---|---|
57732 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4351 | 1.6621 | 0.8634 | [X:[], M:[0.8773], q:[0.3567, 0.6022], qb:[0.5205, 0.4151], phi:[0.3509]] | t^2.11 + t^2.32 + 2*t^2.63 + t^3.05 + t^3.16 + t^3.37 + t^3.68 + t^4.1 + t^4.21 + 3*t^4.42 + t^4.63 + 3*t^4.74 + 2*t^4.95 + t^5. + t^5.1 + 2*t^5.16 + 3*t^5.26 + t^5.37 + t^5.42 + 3*t^5.47 + 2*t^5.68 + t^5.74 + 3*t^5.79 - t^6. - t^4.05/y - t^5.11/y - t^4.05*y - t^5.11*y | detail |