Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

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
6440 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1^2$ + $ M_2\phi_1q_2^2$ + $ M_7\phi_1\tilde{q}_1^2$ + $ M_5M_8$ + $ M_9\phi_1q_2^2$ 0.7092 0.9033 0.7851 [X:[], M:[0.9915, 0.7787, 0.9383, 0.8319, 1.1681, 1.1149, 0.6724, 0.8319, 0.7787], q:[0.6192, 0.3894], qb:[0.4425, 0.7787], phi:[0.4425]] [X:[], M:[[-18], [2], [-13], [-3], [3], [8], [12], [-3], [2]], q:[[17], [1]], qb:[[-4], [2]], phi:[[-4]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_7$, $ M_2$, $ M_9$, $ M_4$, $ M_8$, $ M_3$, $ M_1$, $ M_6$, $ \phi_1q_2\tilde{q}_1$, $ M_7^2$, $ q_1\tilde{q}_2$, $ M_2M_7$, $ M_7M_9$, $ \phi_1q_1q_2$, $ M_4M_7$, $ M_7M_8$, $ \phi_1q_1\tilde{q}_1$, $ M_2^2$, $ M_2M_9$, $ M_9^2$, $ M_2M_4$, $ M_3M_7$, $ M_2M_8$, $ M_4M_9$, $ M_8M_9$, $ \phi_1q_2\tilde{q}_2$, $ M_4^2$, $ M_1M_7$, $ M_4M_8$, $ M_8^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_1^2$, $ M_2M_3$, $ M_3M_9$, $ M_1M_2$, $ M_3M_4$, $ M_3M_8$, $ M_1M_9$, $ M_6M_7$, $ M_1M_4$, $ M_1M_8$, $ M_3^2$, $ M_2M_6$, $ M_6M_9$, $ M_1M_3$, $ M_4M_6$, $ M_6M_8$, $ M_7\phi_1q_2\tilde{q}_1$, $ M_1^2$ . -3 t^2.02 + 2*t^2.34 + 2*t^2.5 + t^2.81 + t^2.97 + t^3.34 + t^3.82 + t^4.03 + t^4.19 + 3*t^4.35 + 3*t^4.51 + 3*t^4.67 + 5*t^4.83 + 4*t^4.99 + t^5.04 + 2*t^5.15 + 3*t^5.31 + t^5.36 + t^5.47 + t^5.63 + 2*t^5.68 + t^5.79 + 2*t^5.84 + t^5.95 - 3*t^6. + t^6.05 + t^6.16 + t^6.21 + 2*t^6.32 + 3*t^6.37 - t^6.48 + 4*t^6.53 + 6*t^6.69 + 7*t^6.85 + 8*t^7.01 + t^7.06 + 8*t^7.17 + 7*t^7.33 + 3*t^7.38 + 7*t^7.49 + 2*t^7.54 + 6*t^7.65 + 2*t^7.7 + 4*t^7.81 + t^7.86 + 4*t^7.97 - t^8.02 + t^8.07 + 3*t^8.13 + t^8.18 + t^8.23 + 3*t^8.28 - 4*t^8.34 + 4*t^8.39 + 2*t^8.44 - 6*t^8.5 + 4*t^8.55 + t^8.6 + 6*t^8.71 + t^8.76 - 3*t^8.81 + 8*t^8.87 + t^8.92 - 4*t^8.97 - t^4.33/y - t^6.34/y - (2*t^6.66)/y - t^6.82/y - t^7.14/y - t^7.3/y + (3*t^7.35)/y + (3*t^7.51)/y + t^7.67/y + (6*t^7.83)/y + (4*t^7.99)/y + (2*t^8.15)/y + (5*t^8.31)/y + (2*t^8.47)/y + t^8.79/y + (2*t^8.84)/y - t^4.33*y - t^6.34*y - 2*t^6.66*y - t^6.82*y - t^7.14*y - t^7.3*y + 3*t^7.35*y + 3*t^7.51*y + t^7.67*y + 6*t^7.83*y + 4*t^7.99*y + 2*t^8.15*y + 5*t^8.31*y + 2*t^8.47*y + t^8.79*y + 2*t^8.84*y g1^12*t^2.02 + 2*g1^2*t^2.34 + (2*t^2.5)/g1^3 + t^2.81/g1^13 + t^2.97/g1^18 + g1^8*t^3.34 + t^3.82/g1^7 + g1^24*t^4.03 + g1^19*t^4.19 + 3*g1^14*t^4.35 + 3*g1^9*t^4.51 + 3*g1^4*t^4.67 + (5*t^4.83)/g1 + (4*t^4.99)/g1^6 + g1^30*t^5.04 + (2*t^5.15)/g1^11 + (3*t^5.31)/g1^16 + g1^20*t^5.36 + t^5.47/g1^21 + t^5.63/g1^26 + 2*g1^10*t^5.68 + t^5.79/g1^31 + 2*g1^5*t^5.84 + t^5.95/g1^36 - 3*t^6. + g1^36*t^6.05 + t^6.16/g1^5 + g1^31*t^6.21 + (2*t^6.32)/g1^10 + 3*g1^26*t^6.37 - t^6.48/g1^15 + 4*g1^21*t^6.53 + 6*g1^16*t^6.69 + 7*g1^11*t^6.85 + 8*g1^6*t^7.01 + g1^42*t^7.06 + 8*g1*t^7.17 + (7*t^7.33)/g1^4 + 3*g1^32*t^7.38 + (7*t^7.49)/g1^9 + 2*g1^27*t^7.54 + (6*t^7.65)/g1^14 + 2*g1^22*t^7.7 + (4*t^7.81)/g1^19 + g1^17*t^7.86 + (4*t^7.97)/g1^24 - g1^12*t^8.02 + g1^48*t^8.07 + (3*t^8.13)/g1^29 + g1^7*t^8.18 + g1^43*t^8.23 + (3*t^8.28)/g1^34 - 4*g1^2*t^8.34 + 4*g1^38*t^8.39 + (2*t^8.44)/g1^39 - (6*t^8.5)/g1^3 + 4*g1^33*t^8.55 + t^8.6/g1^44 + 6*g1^28*t^8.71 + t^8.76/g1^49 - (3*t^8.81)/g1^13 + 8*g1^23*t^8.87 + t^8.92/g1^54 - (4*t^8.97)/g1^18 - t^4.33/(g1^4*y) - (g1^8*t^6.34)/y - (2*t^6.66)/(g1^2*y) - t^6.82/(g1^7*y) - t^7.14/(g1^17*y) - t^7.3/(g1^22*y) + (3*g1^14*t^7.35)/y + (3*g1^9*t^7.51)/y + (g1^4*t^7.67)/y + (6*t^7.83)/(g1*y) + (4*t^7.99)/(g1^6*y) + (2*t^8.15)/(g1^11*y) + (5*t^8.31)/(g1^16*y) + (2*t^8.47)/(g1^21*y) + t^8.79/(g1^31*y) + (2*g1^5*t^8.84)/y - (t^4.33*y)/g1^4 - g1^8*t^6.34*y - (2*t^6.66*y)/g1^2 - (t^6.82*y)/g1^7 - (t^7.14*y)/g1^17 - (t^7.3*y)/g1^22 + 3*g1^14*t^7.35*y + 3*g1^9*t^7.51*y + g1^4*t^7.67*y + (6*t^7.83*y)/g1 + (4*t^7.99*y)/g1^6 + (2*t^8.15*y)/g1^11 + (5*t^8.31*y)/g1^16 + (2*t^8.47*y)/g1^21 + (t^8.79*y)/g1^31 + 2*g1^5*t^8.84*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


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
4811 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ M_3q_1\tilde{q}_1$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_2\tilde{q}_1$ + $ M_4M_5$ + $ \phi_1\tilde{q}_2^2$ + $ M_6\phi_1^2$ + $ M_2\phi_1q_2^2$ + $ M_7\phi_1\tilde{q}_1^2$ + $ M_5M_8$ 0.6915 0.8717 0.7933 [X:[], M:[0.988, 0.7791, 0.9358, 0.8313, 1.1687, 1.1165, 0.6747, 0.8313], q:[0.6225, 0.3896], qb:[0.4418, 0.7791], phi:[0.4418]] t^2.02 + t^2.34 + 2*t^2.49 + t^2.81 + t^2.96 + t^3.35 + t^3.66 + t^3.82 + t^4.05 + t^4.2 + 2*t^4.36 + 3*t^4.52 + t^4.67 + 3*t^4.83 + 4*t^4.99 + t^5.06 + t^5.14 + 2*t^5.3 + t^5.37 + t^5.46 + t^5.61 + 2*t^5.69 + t^5.77 + 2*t^5.84 + t^5.93 - 2*t^6. - t^4.33/y - t^4.33*y detail