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
3487 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}X_{1}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ + ${ }M_{7}^{2}$ 0.5847 0.7249 0.8065 [X:[1.5852], M:[0.926, 1.1704, 0.7331, 1.2444, 0.4148, 0.7556, 1.0], q:[0.2926, 0.7813], qb:[0.463, 0.8039], phi:[0.4148]] [X:[[2]], M:[[10], [4], [-18], [-6], [-2], [6], [0]], q:[[1], [-11]], qb:[[5], [13]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{3}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{1}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{2}^{2}$ ${}$ -1 t^2.199 + t^2.267 + t^2.778 + t^3. + t^3.289 + 2*t^3.511 + t^3.733 + t^4.023 + t^4.399 + t^4.466 + t^4.534 + t^4.756 + t^4.977 + t^5.045 + t^5.199 + t^5.267 + 2*t^5.556 + t^5.711 + 2*t^5.778 + t^5.932 - t^6. + t^6.068 + 3*t^6.289 + t^6.511 + t^6.579 + t^6.598 + t^6.666 + 3*t^6.801 + 2*t^7.023 + t^7.177 + t^7.312 + t^7.399 + t^7.466 + 2*t^7.534 + t^7.756 + 2*t^7.823 + t^7.91 + 3*t^8.045 + t^8.132 - t^8.199 - t^8.267 + 2*t^8.334 + t^8.489 + 2*t^8.556 - 2*t^8.778 + t^8.797 + 2*t^8.846 + t^8.865 - t^4.244/y - t^6.444/y - t^7.023/y + (2*t^7.466)/y + t^7.977/y + (2*t^8.045)/y + t^8.199/y + t^8.267/y + t^8.489/y + t^8.556/y - t^8.643/y + (2*t^8.711)/y + (3*t^8.778)/y + t^8.932/y - t^4.244*y - t^6.444*y - t^7.023*y + 2*t^7.466*y + t^7.977*y + 2*t^8.045*y + t^8.199*y + t^8.267*y + t^8.489*y + t^8.556*y - t^8.643*y + 2*t^8.711*y + 3*t^8.778*y + t^8.932*y t^2.199/g1^18 + g1^6*t^2.267 + g1^10*t^2.778 + t^3. + g1^14*t^3.289 + 2*g1^4*t^3.511 + t^3.733/g1^6 + g1^8*t^4.023 + t^4.399/g1^36 + t^4.466/g1^12 + g1^12*t^4.534 + g1^2*t^4.756 + t^4.977/g1^8 + g1^16*t^5.045 + t^5.199/g1^18 + g1^6*t^5.267 + 2*g1^20*t^5.556 + t^5.711/g1^14 + 2*g1^10*t^5.778 + t^5.932/g1^24 - t^6. + g1^24*t^6.068 + 3*g1^14*t^6.289 + g1^4*t^6.511 + g1^28*t^6.579 + t^6.598/g1^54 + t^6.666/g1^30 + 3*g1^18*t^6.801 + 2*g1^8*t^7.023 + t^7.177/g1^26 + g1^22*t^7.312 + t^7.399/g1^36 + t^7.466/g1^12 + 2*g1^12*t^7.534 + g1^2*t^7.756 + 2*g1^26*t^7.823 + t^7.91/g1^32 + 3*g1^16*t^8.045 + t^8.132/g1^42 - t^8.199/g1^18 - g1^6*t^8.267 + 2*g1^30*t^8.334 + t^8.489/g1^4 + 2*g1^20*t^8.556 - 2*g1^10*t^8.778 + t^8.797/g1^72 + 2*g1^34*t^8.846 + t^8.865/g1^48 - t^4.244/(g1^2*y) - t^6.444/(g1^20*y) - (g1^8*t^7.023)/y + (2*t^7.466)/(g1^12*y) + t^7.977/(g1^8*y) + (2*g1^16*t^8.045)/y + t^8.199/(g1^18*y) + (g1^6*t^8.267)/y + t^8.489/(g1^4*y) + (g1^20*t^8.556)/y - t^8.643/(g1^38*y) + (2*t^8.711)/(g1^14*y) + (3*g1^10*t^8.778)/y + t^8.932/(g1^24*y) - (t^4.244*y)/g1^2 - (t^6.444*y)/g1^20 - g1^8*t^7.023*y + (2*t^7.466*y)/g1^12 + (t^7.977*y)/g1^8 + 2*g1^16*t^8.045*y + (t^8.199*y)/g1^18 + g1^6*t^8.267*y + (t^8.489*y)/g1^4 + g1^20*t^8.556*y - (t^8.643*y)/g1^38 + (2*t^8.711*y)/g1^14 + 3*g1^10*t^8.778*y + (t^8.932*y)/g1^24


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
2902 SU2adj1nf2 ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}X_{1}$ + ${ }M_{7}\phi_{1}q_{1}^{2}$ 0.6388 0.7919 0.8066 [X:[1.6177], M:[0.7844, 1.2353, 0.7449, 1.147, 0.3823, 0.853, 0.696], q:[0.4608, 0.7548], qb:[0.3922, 0.8629], phi:[0.3823]] t^2.088 + t^2.235 + t^2.353 + t^2.559 + t^3.441 + t^3.5 + 2*t^3.706 + t^3.971 + t^4.176 + t^4.323 + t^4.441 + t^4.469 + t^4.588 + t^4.647 + t^4.707 + t^4.794 + t^4.853 + t^4.912 + t^5.118 + t^5.529 + t^5.588 + t^5.676 + 2*t^5.794 + t^5.854 + t^5.941 - 2*t^6. - t^4.147/y - t^4.147*y detail