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$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
46733 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1q_1^2$ + $ M_5\phi_1^2$ 0.6991 0.86 0.8129 [X:[], M:[0.7009, 0.7009, 1.0, 1.0, 1.1495], q:[0.7874, 0.5117], qb:[0.5117, 0.4883], phi:[0.4252]] [X:[], M:[[1, 15], [-1, 1], [-1, -7], [1, 7], [0, -4]], q:[[0, -1], [-1, -14]], qb:[[1, 0], [0, 7]], phi:[[0, 2]]] 2
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_2$, $ M_1$, $ M_3$, $ M_4$, $ q_2\tilde{q}_1$, $ M_5$, $ q_1\tilde{q}_2$, $ M_2^2$, $ M_1M_2$, $ \phi_1\tilde{q}_2^2$, $ M_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2^2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ M_2M_3$, $ M_1M_3$, $ M_2M_4$, $ \phi_1q_1\tilde{q}_2$, $ M_1M_4$, $ \phi_1q_1q_2$, $ M_2q_2\tilde{q}_1$, $ \phi_1q_1\tilde{q}_1$, $ M_2M_5$, $ M_1M_5$ $M_3^2$, $ M_4^2$ -2 2*t^2.1 + 2*t^3. + t^3.07 + t^3.45 + t^3.83 + 4*t^4.21 + 2*t^4.28 + 3*t^4.35 + 4*t^5.1 + 2*t^5.17 + 2*t^5.55 - 2*t^6. + t^6.14 + 6*t^6.31 + 3*t^6.38 + 6*t^6.45 + t^6.52 + 6*t^7.21 + 4*t^7.28 + 4*t^7.35 + 3*t^7.42 + 4*t^7.65 - 4*t^8.1 - t^8.17 + 9*t^8.41 + 6*t^8.48 + 11*t^8.55 + 4*t^8.62 + 5*t^8.69 - t^8.93 - t^4.28/y - (2*t^6.38)/y + t^7.21/y + (4*t^8.1)/y + (4*t^8.17)/y - (3*t^8.48)/y + (2*t^8.55)/y + (2*t^8.93)/y - t^4.28*y - 2*t^6.38*y + t^7.21*y + 4*t^8.1*y + 4*t^8.17*y - 3*t^8.48*y + 2*t^8.55*y + 2*t^8.93*y (g2*t^2.1)/g1 + g1*g2^15*t^2.1 + t^3./(g1*g2^7) + g1*g2^7*t^3. + t^3.07/g2^14 + t^3.45/g2^4 + g2^6*t^3.83 + (g2^2*t^4.21)/g1^2 + 2*g2^16*t^4.21 + g1^2*g2^30*t^4.21 + t^4.28/(g1*g2^5) + g1*g2^9*t^4.28 + t^4.35/(g1^2*g2^26) + t^4.35/g2^12 + g1^2*g2^2*t^4.35 + t^5.1/(g1^2*g2^6) + 2*g2^8*t^5.1 + g1^2*g2^22*t^5.1 + t^5.17/(g1*g2^13) + g1*g2*t^5.17 + t^5.55/(g1*g2^3) + g1*g2^11*t^5.55 - 2*t^6. + t^6.14/g2^28 + (g2^3*t^6.31)/g1^3 + (2*g2^17*t^6.31)/g1 + 2*g1*g2^31*t^6.31 + g1^3*g2^45*t^6.31 + t^6.38/(g1^2*g2^4) + g2^10*t^6.38 + g1^2*g2^24*t^6.38 + t^6.45/(g1^3*g2^25) + (2*t^6.45)/(g1*g2^11) + 2*g1*g2^3*t^6.45 + g1^3*g2^17*t^6.45 + t^6.52/g2^18 + t^7.21/(g1^3*g2^5) + (2*g2^9*t^7.21)/g1 + 2*g1*g2^23*t^7.21 + g1^3*g2^37*t^7.21 + t^7.28/(g1^2*g2^12) + 2*g2^2*t^7.28 + g1^2*g2^16*t^7.28 + t^7.35/(g1^3*g2^33) + t^7.35/(g1*g2^19) + (g1*t^7.35)/g2^5 + g1^3*g2^9*t^7.35 + t^7.42/(g1^2*g2^40) + t^7.42/g2^26 + (g1^2*t^7.42)/g2^12 + t^7.65/(g1^2*g2^2) + 2*g2^12*t^7.65 + g1^2*g2^26*t^7.65 - (2*g2*t^8.1)/g1 - 2*g1*g2^15*t^8.1 - t^8.17/g2^6 + (g2^4*t^8.41)/g1^4 + (2*g2^18*t^8.41)/g1^2 + 3*g2^32*t^8.41 + 2*g1^2*g2^46*t^8.41 + g1^4*g2^60*t^8.41 + t^8.48/(g1^3*g2^3) + (2*g2^11*t^8.48)/g1 + 2*g1*g2^25*t^8.48 + g1^3*g2^39*t^8.48 + t^8.55/(g1^4*g2^24) + (3*t^8.55)/(g1^2*g2^10) + 3*g2^4*t^8.55 + 3*g1^2*g2^18*t^8.55 + g1^4*g2^32*t^8.55 + t^8.62/(g1^3*g2^31) + t^8.62/(g1*g2^17) + (g1*t^8.62)/g2^3 + g1^3*g2^11*t^8.62 + t^8.69/(g1^4*g2^52) + t^8.69/(g1^2*g2^38) + t^8.69/g2^24 + (g1^2*t^8.69)/g2^10 + g1^4*g2^4*t^8.69 - g2^14*t^8.93 - (g2^2*t^4.28)/y - (g2^3*t^6.38)/(g1*y) - (g1*g2^17*t^6.38)/y + (g2^16*t^7.21)/y + t^8.1/(g1^2*g2^6*y) + (2*g2^8*t^8.1)/y + (g1^2*g2^22*t^8.1)/y + (2*t^8.17)/(g1*g2^13*y) + (2*g1*g2*t^8.17)/y - (g2^4*t^8.48)/(g1^2*y) - (g2^18*t^8.48)/y - (g1^2*g2^32*t^8.48)/y + t^8.55/(g1*g2^3*y) + (g1*g2^11*t^8.55)/y + (g2^7*t^8.93)/(g1*y) + (g1*g2^21*t^8.93)/y - g2^2*t^4.28*y - (g2^3*t^6.38*y)/g1 - g1*g2^17*t^6.38*y + g2^16*t^7.21*y + (t^8.1*y)/(g1^2*g2^6) + 2*g2^8*t^8.1*y + g1^2*g2^22*t^8.1*y + (2*t^8.17*y)/(g1*g2^13) + 2*g1*g2*t^8.17*y - (g2^4*t^8.48*y)/g1^2 - g2^18*t^8.48*y - g1^2*g2^32*t^8.48*y + (t^8.55*y)/(g1*g2^3) + g1*g2^11*t^8.55*y + (g2^7*t^8.93*y)/g1 + g1*g2^21*t^8.93*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
48290 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1q_1^2$ + $ M_5\phi_1^2$ + $ M_6q_2\tilde{q}_1$ 0.7038 0.8701 0.8089 [X:[], M:[0.6699, 0.6699, 1.0, 1.0, 1.165, 0.9223], q:[0.7913, 0.5388], qb:[0.5388, 0.4612], phi:[0.4175]] 2*t^2.01 + t^2.77 + 2*t^3. + t^3.5 + t^3.76 + 4*t^4.02 + 2*t^4.25 + 3*t^4.49 + 2*t^4.78 + 4*t^5.01 + 2*t^5.5 + t^5.53 + 2*t^5.77 - 2*t^6. - t^4.25/y - t^4.25*y detail


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


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


Previous Theory

The previous fixed point before deforming to get the chosen fixed point.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
46340 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_3M_4$ + $ \phi_1q_1^2$ 0.7123 0.8829 0.8068 [X:[], M:[0.6935, 0.6935, 1.0, 1.0], q:[0.7883, 0.5182], qb:[0.5182, 0.4818], phi:[0.4234]] 2*t^2.08 + t^2.54 + 2*t^3. + t^3.11 + t^3.81 + 4*t^4.16 + 2*t^4.27 + 3*t^4.38 + 2*t^4.62 + 5*t^5.08 + 2*t^5.19 + 2*t^5.54 + t^5.65 - 2*t^6. - t^4.27/y - t^4.27*y detail