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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60054 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.4652 | 1.6705 | 0.8771 | [X:[1.341], M:[0.7117, 0.9588], q:[0.5843, 0.5019], qb:[0.4569, 0.4799], phi:[0.3295]] | [X:[[0, 2]], M:[[3, -16], [-3, 17]], q:[[2, -11], [-4, 23]], 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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${}M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}$ | -3 | t^2.14 + 2*t^2.88 + t^2.95 + t^2.97 + t^3.19 + t^3.93 + t^4.02 + t^4.11 + t^4.18 + t^4.27 + t^4.85 + t^4.92 + 2*t^5.01 + t^5.08 + 2*t^5.1 + 2*t^5.17 + t^5.24 + t^5.33 + 3*t^5.75 + 2*t^5.82 + 2*t^5.84 + t^5.89 + t^5.91 - 3*t^6. + 2*t^6.07 + t^6.14 + 3*t^6.16 + t^6.23 + t^6.32 + t^6.39 + t^6.41 + 2*t^6.81 + t^6.88 + 3*t^6.9 - t^6.92 + t^6.97 + 2*t^6.99 + 2*t^7.06 + 2*t^7.08 + 2*t^7.13 + 4*t^7.15 + 3*t^7.22 + t^7.24 + t^7.28 + 2*t^7.3 + 2*t^7.37 + t^7.46 + t^7.48 + 2*t^7.73 + 3*t^7.8 + 2*t^7.87 + 2*t^7.89 - t^7.91 + 2*t^7.96 + 2*t^7.98 + t^8.03 + 5*t^8.05 + t^8.07 + 5*t^8.11 - t^8.14 + t^8.18 + 3*t^8.2 + t^8.27 + 3*t^8.29 + 3*t^8.36 + t^8.43 + t^8.45 + t^8.52 + t^8.54 - t^8.56 + 3*t^8.63 + 3*t^8.7 + 3*t^8.72 + 2*t^8.77 + 3*t^8.79 - t^8.81 + t^8.84 + 2*t^8.86 - 7*t^8.88 - 2*t^8.97 + t^8.97/y^2 - t^3.99/y - t^4.98/y - t^6.12/y - (2*t^6.86)/y - t^6.93/y - t^6.95/y - t^7.11/y - t^7.18/y - t^7.85/y - t^7.92/y - t^7.94/y + (2*t^8.01)/y + t^8.08/y + t^8.1/y - t^8.17/y - t^8.26/y + t^8.33/y + t^8.75/y + (2*t^8.82)/y + (2*t^8.84)/y - t^3.99*y - t^4.98*y - t^6.12*y - 2*t^6.86*y - t^6.93*y - t^6.95*y - t^7.11*y - t^7.18*y - t^7.85*y - t^7.92*y - t^7.94*y + 2*t^8.01*y + t^8.08*y + t^8.1*y - t^8.17*y - t^8.26*y + t^8.33*y + t^8.75*y + 2*t^8.82*y + 2*t^8.84*y + t^8.97*y^2 | (g1^3*t^2.14)/g2^16 + (2*g2^17*t^2.88)/g1^3 + (g2^23*t^2.95)/g1^3 + t^2.97/g2^3 + (g1^3*t^3.19)/g2^11 + (g2^22*t^3.93)/g1^3 + g2^2*t^4.02 + (g1^3*t^4.11)/g2^18 + (g1^3*t^4.18)/g2^12 + (g1^6*t^4.27)/g2^32 + (g2^15*t^4.85)/g1^3 + (g2^21*t^4.92)/g1^3 + 2*g2*t^5.01 + g2^7*t^5.08 + (2*g1^3*t^5.1)/g2^19 + (2*g1^3*t^5.17)/g2^13 + (g1^3*t^5.24)/g2^7 + (g1^6*t^5.33)/g2^27 + (3*g2^34*t^5.75)/g1^6 + (2*g2^40*t^5.82)/g1^6 + (2*g2^14*t^5.84)/g1^3 + (g2^46*t^5.89)/g1^6 + (g2^20*t^5.91)/g1^3 - 3*t^6. + 2*g2^6*t^6.07 + g2^12*t^6.14 + (3*g1^3*t^6.16)/g2^14 + (g1^3*t^6.23)/g2^8 + (g1^6*t^6.32)/g2^28 + (g1^6*t^6.39)/g2^22 + (g1^9*t^6.41)/g2^48 + (2*g2^39*t^6.81)/g1^6 + (g2^45*t^6.88)/g1^6 + (3*g2^19*t^6.9)/g1^3 - t^6.92/g2^7 + (g2^25*t^6.97)/g1^3 + (2*t^6.99)/g2 + 2*g2^5*t^7.06 + (2*g1^3*t^7.08)/g2^21 + 2*g2^11*t^7.13 + (4*g1^3*t^7.15)/g2^15 + (3*g1^3*t^7.22)/g2^9 + (g1^6*t^7.24)/g2^35 + (g1^3*t^7.28)/g2^3 + (2*g1^6*t^7.3)/g2^29 + (2*g1^6*t^7.37)/g2^23 + (g1^9*t^7.46)/g2^43 + (g2^66*t^7.48)/g1^12 + (2*g2^32*t^7.73)/g1^6 + (3*g2^38*t^7.8)/g1^6 + (2*g2^44*t^7.87)/g1^6 + (2*g2^18*t^7.89)/g1^3 - t^7.91/g2^8 + (2*g2^24*t^7.96)/g1^3 + (2*t^7.98)/g2^2 + (g2^30*t^8.03)/g1^3 + 5*g2^4*t^8.05 + (g1^3*t^8.07)/g2^22 + 5*g2^10*t^8.11 - (g1^3*t^8.14)/g2^16 + g2^16*t^8.18 + (3*g1^3*t^8.2)/g2^10 + (g1^3*t^8.27)/g2^4 + (3*g1^6*t^8.29)/g2^30 + (3*g1^6*t^8.36)/g2^24 + (g1^6*t^8.43)/g2^18 + (g1^9*t^8.45)/g2^44 + (g1^9*t^8.52)/g2^38 + (g1^12*t^8.54)/g2^64 - (g2^45*t^8.56)/g1^9 + (3*g2^51*t^8.63)/g1^9 + (3*g2^57*t^8.7)/g1^9 + (3*g2^31*t^8.72)/g1^6 + (2*g2^63*t^8.77)/g1^9 + (3*g2^37*t^8.79)/g1^6 - (g2^11*t^8.81)/g1^3 + (g2^69*t^8.84)/g1^9 + (2*g2^43*t^8.86)/g1^6 - (7*g2^17*t^8.88)/g1^3 - (2*t^8.97)/g2^3 + t^8.97/(g2^3*y^2) - t^3.99/(g2*y) - t^4.98/(g2^2*y) - (g1^3*t^6.12)/(g2^17*y) - (2*g2^16*t^6.86)/(g1^3*y) - (g2^22*t^6.93)/(g1^3*y) - t^6.95/(g2^4*y) - (g1^3*t^7.11)/(g2^18*y) - (g1^3*t^7.18)/(g2^12*y) - (g2^15*t^7.85)/(g1^3*y) - (g2^21*t^7.92)/(g1^3*y) - t^7.94/(g2^5*y) + (2*g2*t^8.01)/y + (g2^7*t^8.08)/y + (g1^3*t^8.1)/(g2^19*y) - (g1^3*t^8.17)/(g2^13*y) - (g1^6*t^8.26)/(g2^33*y) + (g1^6*t^8.33)/(g2^27*y) + (g2^34*t^8.75)/(g1^6*y) + (2*g2^40*t^8.82)/(g1^6*y) + (2*g2^14*t^8.84)/(g1^3*y) - (t^3.99*y)/g2 - (t^4.98*y)/g2^2 - (g1^3*t^6.12*y)/g2^17 - (2*g2^16*t^6.86*y)/g1^3 - (g2^22*t^6.93*y)/g1^3 - (t^6.95*y)/g2^4 - (g1^3*t^7.11*y)/g2^18 - (g1^3*t^7.18*y)/g2^12 - (g2^15*t^7.85*y)/g1^3 - (g2^21*t^7.92*y)/g1^3 - (t^7.94*y)/g2^5 + 2*g2*t^8.01*y + g2^7*t^8.08*y + (g1^3*t^8.1*y)/g2^19 - (g1^3*t^8.17*y)/g2^13 - (g1^6*t^8.26*y)/g2^33 + (g1^6*t^8.33*y)/g2^27 + (g2^34*t^8.75*y)/g1^6 + (2*g2^40*t^8.82*y)/g1^6 + (2*g2^14*t^8.84*y)/g1^3 + (t^8.97*y^2)/g2^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57693 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.4621 | 1.6651 | 0.8781 | [X:[1.3424], M:[0.6976], q:[0.5746, 0.5219], qb:[0.4517, 0.479], phi:[0.3288]] | t^2.09 + t^2.92 + t^2.96 + t^3. + t^3.08 + t^3.16 + t^3.99 + t^4.03 + t^4.07 + t^4.15 + t^4.19 + t^4.89 + t^4.98 + t^5.01 + 2*t^5.05 + t^5.1 + 2*t^5.13 + t^5.17 + t^5.22 + t^5.25 + t^5.84 + t^5.88 + t^5.92 + t^5.96 - 2*t^6. - t^3.99/y - t^4.97/y - t^3.99*y - t^4.97*y | detail |